Optical image capturing system

ABSTRACT

An optical image capturing system includes, along the optical axis in order from an object side to an image side, a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens. At least one lens among the first to the sixth lenses has positive refractive power. The seventh lens has negative refractive power, wherein both surfaces thereof can be aspheric, and at least one surface thereof has an inflection point. The lenses in the optical image capturing system which have refractive power include the first to the seventh lenses. The optical image capturing system can increase aperture value and improve the imaging quality for use in compact cameras.

BACKGROUND OF THE INVENTION 1. Technical Field

The present invention generally relates to an optical system, and more particularly to a compact optical image capturing system for an electronic device.

2. Description of Related Art

In recent years, with the rise of portable electronic devices having camera functionalities, the demand for an optical image capturing system is raised gradually. The image sensing device of the ordinary photographing camera is commonly selected from charge coupled device (CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor). Also, as advanced semiconductor manufacturing technology enables the minimization of the pixel size of the image sensing device, the development of the optical image capturing system towards the field of high pixels. Therefore, the requirement for high imaging quality is rapidly raised.

The conventional optical system of the portable electronic device usually has five or sixth lenses. However, the optical system is asked to take pictures in a dark environment, in other words, the optical system is asked to have a large aperture. The conventional optical system provides high optical performance as required.

It is an important issue to increase the quantity of light entering the lens. Also, the modern lens is also asked to have several characters, including high image quality.

BRIEF SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an optical image capturing system and an optical image capturing lens which use combination of refractive powers, convex and concave surfaces of seven-piece optical lenses (the convex or concave surface in the disclosure denotes the geometrical shape of an image-side surface or an object-side surface of each lens on an optical axis) to increase the quantity of incoming light of the optical image capturing system, and to improve imaging quality for image formation, so as to be applied to minimized electronic products.

The term and its definition to the lens parameter in the embodiment of the present are shown as below for further reference.

The lens parameter related to a length or a height in the lens:

For visible spectrum, the present invention may adopt the wavelength of 555 nm as the primary reference wavelength and the basis for the measurement of focus shift; for infrared spectrum (700-1300 nm), the present invention may adopt the wavelength of 940 nm as the primary reference wavelength and the basis for the measurement of focus shift.

The optical image capturing system includes an image plane specifically for the infrared light which is perpendicular to the optical axis, wherein the through-focus modulation transfer rate (value of MTF) at a first spatial frequency has a maximum value in the central of field of view of the image plane specifically for the infrared light, wherein the first spatial frequency is denoted by SP1, which satisfies the following condition: SP1≤440 cycles/mm Preferably, the first spatial frequency satisfies the following condition: SP1≤220 cycles/mm.

A maximum height for image formation of the optical image capturing system is denoted by HOI. A height of the optical image capturing system is denoted by HOS. A distance from the object-side surface of the first lens to the image-side surface of the seventh lens is denoted by InTL. A distance between the aperture and the image plane specifically for the infrared light is denoted by InS. A distance from the first lens to the second lens is denoted by IN12 (instance). A central thickness of the first lens of the optical image capturing system on the optical axis is denoted by TP1 (instance).

The lens parameter related to a material in the lens:

An Abbe number of the first lens in the optical image capturing system is denoted by NA1 (instance). A refractive index of the first lens is denoted by Nd1 (instance).

The lens parameter related to a view angle of the lens:

A view angle is denoted by AF. Half of the view angle is denoted by HAF. A major light angle is denoted by MRA.

The lens parameter related to exit/entrance pupil in the lens:

An entrance pupil diameter of the optical image capturing system is denoted by HEP. An exit pupil diameter of the image-side surface of the seventh lens is denoted by HXP. For any surface of any lens, a maximum effective half diameter (EHD) is a perpendicular distance between an optical axis and a crossing point on the surface where the incident light with a maximum viewing angle of the system passing the very edge of the entrance pupil. For example, the maximum effective half diameter of the object-side surface of the first lens is denoted by EHD11, the maximum effective half diameter of the image-side surface of the first lens is denoted by EHD12, the maximum effective half diameter of the object-side surface of the second lens is denoted by EHD21, the maximum effective half diameter of the image-side surface of the second lens is denoted by EHD22, and so on.

The lens parameter related to a depth of the lens shape:

A displacement from a point on the object-side surface of the seventh lens, which is passed through by the optical axis, to a point on the optical axis, where a projection of the maximum effective semi diameter of the object-side surface of the seventh lens ends, is denoted by InRS71 (the depth of the maximum effective semi diameter). A displacement from a point on the image-side surface of the seventh lens, which is passed through by the optical axis, to a point on the optical axis, where a projection of the maximum effective semi diameter of the image-side surface of the seventh lens ends, is denoted by InRS72 (the depth of the maximum effective semi diameter). The depth of the maximum effective semi diameter (sinkage) on the object-side surface or the image-side surface of any other lens is denoted in the same manner.

The lens parameter related to the lens shape:

A critical point C is a tangent point on a surface of a specific lens, and the tangent point is tangent to a plane perpendicular to the optical axis and the tangent point cannot be a crossover point on the optical axis. Following the above description, a distance perpendicular to the optical axis between a critical point C51 on the object-side surface of the fifth lens and the optical axis is HVT51 (instance), and a distance perpendicular to the optical axis between a critical point C52 on the image-side surface of the fifth lens and the optical axis is HVT52 (instance). A distance perpendicular to the optical axis between a critical point C61 on the object-side surface of the sixth lens and the optical axis is HVT61 (instance), and a distance perpendicular to the optical axis between a critical point C62 on the image-side surface of the sixth lens and the optical axis is HVT62 (instance). A distance perpendicular to the optical axis between a critical point on the object-side or image-side surface of other lenses, such as the seventh lens, the optical axis is denoted in the same manner.

The object-side surface of the seventh lens has one inflection point IF711 which is nearest to the optical axis, and the sinkage value of the inflection point IF711 is denoted by SGI711 (instance). A distance perpendicular to the optical axis between the inflection point IF711 and the optical axis is HIF711 (instance). The image-side surface of the seventh lens has one inflection point IF721 which is nearest to the optical axis, and the sinkage value of the inflection point IF721 is denoted by SGI721 (instance). A distance perpendicular to the optical axis between the inflection point IF721 and the optical axis is HIF721 (instance).

The object-side surface of the seventh lens has one inflection point IF712 which is the second nearest to the optical axis, and the sinkage value of the inflection point IF712 is denoted by SGI712 (instance). A distance perpendicular to the optical axis between the inflection point IF712 and the optical axis is HIF712 (instance). The image-side surface of the seventh lens has one inflection point IF722 which is the second nearest to the optical axis, and the sinkage value of the inflection point IF722 is denoted by SGI722 (instance). A distance perpendicular to the optical axis between the inflection point IF722 and the optical axis is HIF722 (instance).

The object-side surface of the seventh lens has one inflection point IF713 which is the third nearest to the optical axis, and the sinkage value of the inflection point IF713 is denoted by SGI713 (instance). A distance perpendicular to the optical axis between the inflection point IF713 and the optical axis is HIF713 (instance). The image-side surface of the seventh lens has one inflection point IF723 which is the third nearest to the optical axis, and the sinkage value of the inflection point IF723 is denoted by SGI723 (instance). A distance perpendicular to the optical axis between the inflection point IF723 and the optical axis is HIF723 (instance).

The object-side surface of the seventh lens has one inflection point IF714 which is the fourth nearest to the optical axis, and the sinkage value of the inflection point IF714 is denoted by SGI714 (instance). A distance perpendicular to the optical axis between the inflection point IF714 and the optical axis is HIF714 (instance). The image-side surface of the seventh lens has one inflection point IF724 which is the fourth nearest to the optical axis, and the sinkage value of the inflection point IF724 is denoted by SGI724 (instance). A distance perpendicular to the optical axis between the inflection point IF724 and the optical axis is HIF724 (instance).

An inflection point, a distance perpendicular to the optical axis between the inflection point and the optical axis, and a sinkage value thereof on the object-side surface or image-side surface of other lenses is denoted in the same manner.

The lens parameter related to an aberration:

Optical distortion for image formation in the optical image capturing system is denoted by ODT. TV distortion for image formation in the optical image capturing system is denoted by TDT. Further, the range of the aberration offset for the view of image formation may be limited to 50%-100% field. An offset of the spherical aberration is denoted by DFS. An offset of the coma aberration is denoted by DFC.

A modulation transfer function (MTF) graph of an optical image capturing system is used to test and evaluate the contrast and sharpness of the generated images. The vertical axis of the coordinate system of the MTF graph represents the contrast transfer rate, of which the value is between 0 and 1, and the horizontal axis of the coordinate system represents the spatial frequency, of which the unit is cycles/mm or 1 p/mm, i.e., line pairs per millimeter. Theoretically, a perfect optical image capturing system can present all detailed contrast and every line of an object in an image. However, the contrast transfer rate of a practical optical image capturing system along a vertical axis thereof would be less than 1. In addition, peripheral areas in an image would have a poorer realistic effect than a center area thereof has. For infrared spectrum, the values of MTF in the spatial frequency of 55 cycles/mm at the optical axis, 0.3 field of view, and 0.7 field of view on an image plane specifically for the infrared light are respectively denoted by MTFE0, MTFE3, and MTFE7; the values of MTF in the spatial frequency of 110 cycles/mm at the optical axis, 0.3 field of view, and 0.7 field of view on an image plane are respectively denoted by MTFQ0, MTFQ3, and MTFQ7; the values of MTF in the spatial frequency of 220 cycles/mm at the optical axis, 0.3 field of view, and 0.7 field of view on an image plane are respectively denoted by MTFH0, MTFH3, and MTFH7; the values of MTF in the spatial frequency of 440 cycles/mm at the optical axis, 0.3 field of view, and 0.7 field of view on the image plane are respectively denoted by MTF0, MTF3, and MTF7. The three aforementioned fields of view respectively represent the center, the inner field of view, and the outer field of view of a lens, and, therefore, can be used to evaluate the performance of an optical image capturing system. If the optical image capturing system provided in the present invention corresponds to photosensitive components which provide pixels having a size no large than 1.12 micrometer, a quarter of the spatial frequency, a half of the spatial frequency (half frequency), and the full spatial frequency (full frequency) of the MTF diagram are respectively at least 110 cycles/mm, 220 cycles/mm and 440 cycles/mm.

If an optical image capturing system is required to be able also to image for infrared spectrum, e.g., to be used in low-light environments, then the optical image capturing system should be workable in wavelengths of 850 nm to 960 nm. Since the main function for an optical image capturing system used in low-light environment is to distinguish the shape of objects by light and shade, which does not require high resolution, it is appropriate to only use spatial frequency less than 110 cycles/mm for evaluating the performance of optical image capturing system in the infrared spectrum.

The present invention provides an optical image capturing system, wherein the seventh lens thereof is provided with an inflection point at the object-side surface or at the image-side surface to adjust the incident angle of each view field and modify the ODT and the TDT. In addition, the surfaces of the seventh lens are capable of modifying the optical path to improve the imagining quality.

The optical image capturing system of the present invention includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane specifically for the infrared light in order along an optical axis from an object side to an image side. The first lens to the seventh lens all have refractive power. The optical image capturing system satisfies: 0.5≤f/HEP≤1.8;0 deg<HAF≤60 deg; and 0.5≤SETP/STP<1;

where f1, f2, f3, f4, f5, f6, and f7 are respectively a focal length of the first lens to the seventh lens; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HXP is an exit pupil diameter of the image-side surface of the seventh lens; HOS is a distance between the object-side surface of the first lens and the image plane specifically for the infrared light; HAF is a half of the maximum field angle of the optical image capturing system; HOI is a maximum height for image formation perpendicular to the optical axis on the image plane specifically for the infrared light; ETP1, ETP2, ETP3, ETP4, ETP5, ETP6, and ETP7 are respectively a thickness in parallel with the optical axis at a height of ½ HXP of the first lens to the seventh lens, wherein SETP is a sum of the aforementioned ETP1 to ETP7; TP1, TP2, TP3, TP4, TP5, TP6, and TP7 are respectively a thickness at the optical axis of the first lens to the seventh lens, wherein STP is a sum of the aforementioned TP1 to TP7.

The present invention further provides an optical image capturing system, including a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane specifically for the infrared light, in order along an optical axis from an object side to an image side. At least one surface of at least one lens among the first lens to the seventh lens has at least an inflection point thereon. The optical image capturing system satisfies: 0.5≤f/HEP≤1.5;0 deg<HAF≤50 deg; and 0.2≤EIN/ETL<1;

where f1, f2, f3, f4, f5, f6, and f7 are respectively a focal length of the first lens to the seventh lens; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HXP is an exit pupil diameter of the image-side surface of the seventh lens; HOS is a distance between the object-side surface of the first lens and the image plane; InTL is a distance from the object-side surface of the first lens to the image-side surface of the seventh lens on the optical axis; HAF is a half of the maximum field angle of the optical image capturing system; ETL is a distance in parallel with the optical axis between a coordinate point at a height of ½ HEP on the object-side surface of the first lens and the image plane specifically for the infrared light; EIN is a distance in parallel with the optical axis between the coordinate point at the height of ½ HEP on the object-side surface of the first lens and a coordinate point at a height of ½ HEP on the image-side surface of the seventh lens.

The present invention further provides an optical image capturing system, including a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane specifically for the infrared light, in order along an optical axis from an object side to an image side. The number of the lenses having refractive power in the optical image capturing system is seven. At least one surface of at least two lenses among the first lens to the seventh lens has at least an inflection point thereon. The optical image capturing system satisfies: 0.5≤f/HEP≤1.3;10 deg≤HAF≤45 deg; and 0.2≤SETP/STP<1;

where f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HAF is a half of the maximum field angle of the optical image capturing system; HOI is a maximum height for image formation perpendicular to the optical axis on the image plane specifically for the infrared light; ETP1, ETP2, ETP3, ETP4, ETP5, ETP6, and ETP7 are respectively a thickness in parallel with the optical axis at a height of ½ HEP of the first lens to the seventh lens, wherein SETP is a sum of the aforementioned ETP1 to ETP7; TP1, TP2, TP3, TP4, TP5, TP6, and TP7 are respectively a central thickness on the optical axis of the first lens to the seventh lens, wherein STP is a sum of the aforementioned TP1 to TP7.

For any lens, the thickness at the height of a half of the entrance pupil diameter (HEP) particularly affects the ability of correcting aberration and differences between optical paths of light in different fields of view of the common region of each field of view of light within the covered range at the height of a half of the entrance pupil diameter (HEP). With greater thickness, the ability to correct aberration is better. However, the difficulty of manufacturing increases as well. Therefore, the thickness at the height of a half of the entrance pupil diameter (HEP) of any lens has to be controlled. The ratio between the thickness (ETP) at the height of a half of the entrance pupil diameter (HEP) and the thickness (TP) of any lens on the optical axis (i.e., ETP/TP) has to be particularly controlled. For example, the thickness at the height of a half of the entrance pupil diameter (HEP) of the first lens is denoted by ETP1, the thickness at the height of a half of the entrance pupil diameter (HEP) of the second lens is denoted by ETP2, and the thickness at the height of a half of the entrance pupil diameter (HEP) of any other lens in the optical image capturing system is denoted in the same manner. The optical image capturing system of the present invention satisfies: 0.3≤SETP/EIN<1;

where SETP is the sum of the aforementioned ETP1 to ETP5.

In order to enhance the ability of correcting aberration and to lower the difficulty of manufacturing at the same time, the ratio between the thickness (ETP) at the height of a half of the entrance pupil diameter (HEP) and the thickness (TP) of any lens on the optical axis (i.e., ETP/TP) has to be particularly controlled. For example, the thickness at the height of a half of the entrance pupil diameter (HEP) of the first lens is denoted by ETP1, the thickness of the first lens on the optical axis is TP1, and the ratio between these two parameters is ETP1/TP1; the thickness at the height of a half of the entrance pupil diameter (HEP) of the first lens is denoted by ETP2, the thickness of the second lens on the optical axis is TP2, and the ratio between these two parameters is ETP2/TP2. The ratio between the thickness at the height of a half of the entrance pupil diameter (HEP) and the thickness of any other lens in the optical image capturing system is denoted in the same manner. The optical image capturing system of the present invention satisfies: 0.2≤ETP/TP≤3.

The horizontal distance between two neighboring lenses at the height of a half of the entrance pupil diameter (HEP) is denoted by ED, wherein the aforementioned horizontal distance (ED) is parallel to the optical axis of the optical image capturing system, and particularly affects the ability of correcting aberration and differences between optical paths of light in different fields of view of the common region of each field of view of light at the height of a half of the entrance pupil diameter (HEP). With longer distance, the ability to correct aberration is potential to be better. However, the difficulty of manufacturing increases, and the feasibility of “slightly shorten” the length of the optical image capturing system is limited as well. Therefore, the horizontal distance (ED) between two specific neighboring lenses at the height of a half of the entrance pupil diameter (HEP) has to be controlled.

In order to enhance the ability of correcting aberration and to lower the difficulty of “slightly shorten” the length of the optical image capturing system at the same time, the ratio between the horizontal distance (ED) between two neighboring lenses at the height of a half of the entrance pupil diameter (HEP) and the parallel distance (IN) between these two neighboring lens on the optical axis (i.e., ED/IN) has to be particularly controlled. For example, the horizontal distance between the first lens and the second lens at the height of a half of the entrance pupil diameter (HEP) is denoted by ED12, the horizontal distance between the first lens and the second lens on the optical axis is denoted by IN12, and the ratio between these two parameters is ED12/IN12; the horizontal distance between the second lens and the third lens at the height of a half of the entrance pupil diameter (HEP) is denoted by ED23, the horizontal distance between the second lens and the third lens on the optical axis is denoted by IN23, and the ratio between these two parameters is ED23/IN23. The ratio between the horizontal distance between any two neighboring lenses at the height of a half of the entrance pupil diameter (HEP) and the horizontal distance between these two neighboring lenses on the optical axis is denoted in the same manner.

The horizontal distance in parallel with the optical axis between a coordinate point at the height of ½ HEP on the image-side surface of the seventh lens and image plane specifically for the infrared light is denoted by EBL. The horizontal distance in parallel with the optical axis between the point on the image-side surface of the seventh lens where the optical axis passes through and the image plane specifically for the infrared light is denoted by BL. To enhance the ability to correct aberration and to preserve more space for other optical components, the optical image capturing system of the present invention can satisfy 0.2≤EBL/BL≤1.5. The optical image capturing system can further include a filtering component, which is provided between the seventh lens and the image plane specifically for the infrared light, wherein the horizontal distance in parallel with the optical axis between the coordinate point at the height of ½ HEP on the image-side surface of the seventh lens and the filtering component is denoted by EIR, and the horizontal distance in parallel with the optical axis between the point on the image-side surface of the seventh lens where the optical axis passes through and the filtering component is denoted by PIR. The optical image capturing system of the present invention can satisfy 0.1≤EIR/PIR≤1.

In an embodiment, a height of the optical image capturing system (HOS) can be reduced while |f1|>|f7|.

In an embodiment, when the lenses satisfy |f2|+|f3|+|f4|+|f5|+|f6| and |f1|+|f7|, at least one lens among the second to the sixth lenses could have weak positive refractive power or weak negative refractive power. Herein the weak refractive power means the absolute value of the focal length of one specific lens is greater than 10. When at least one lens among the second to the sixth lenses has weak positive refractive power, it may share the positive refractive power of the first lens, and on the contrary, when at least one lens among the second to the sixth lenses has weak negative refractive power, it may fine tune and correct the aberration of the system.

In an embodiment, the seventh lens could have negative refractive power, and an image-side surface thereof is concave, it may reduce back focal length and size. Besides, the seventh lens can have at least an inflection point on at least a surface thereof, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

The present invention will be best understood by referring to the following detailed description of some illustrative embodiments in conjunction with the accompanying drawings, in which

FIG. 1A is a schematic diagram of a first embodiment of the present invention;

FIG. 1B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the first embodiment of the present application;

FIG. 1C shows a feature map of modulation transformation of the optical image capturing system of the first embodiment of the present application in infrared spectrum;

FIG. 2A is a schematic diagram of a second embodiment of the present invention;

FIG. 2B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the second embodiment of the present application;

FIG. 2C shows a feature map of modulation transformation of the optical image capturing system of the second embodiment of the present application in infrared spectrum;

FIG. 3A is a schematic diagram of a third embodiment of the present invention;

FIG. 3B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the third embodiment of the present application;

FIG. 3C shows a feature map of modulation transformation of the optical image capturing system of the third embodiment of the present application in infrared spectrum;

FIG. 4A is a schematic diagram of a fourth embodiment of the present invention;

FIG. 4B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the fourth embodiment of the present application;

FIG. 4C shows a feature map of modulation transformation of the optical image capturing system of the fourth embodiment in infrared spectrum;

FIG. 5A is a schematic diagram of a fifth embodiment of the present invention;

FIG. 5B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the fifth embodiment of the present application;

FIG. 5C shows a feature map of modulation transformation of the optical image capturing system of the fifth embodiment of the present application in infrared spectrum;

FIG. 6A is a schematic diagram of a sixth embodiment of the present invention;

FIG. 6B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the sixth embodiment of the present application; and

FIG. 6C shows a feature map of modulation transformation of the optical image capturing system of the sixth embodiment of the present application in infrared spectrum.

DETAILED DESCRIPTION OF THE INVENTION

An optical image capturing system of the present invention includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane specifically for the infrared light from an object side to an image side. The optical image capturing system further is provided with an image sensor at an image plane specifically for the infrared light. Image heights in the following embodiments are all almost 3.91 mm.

The optical image capturing system could work in three infrared light wavelengths, including 850 nm, 940 nm, and 960 nm, wherein 960 nm is the main reference wavelength and is the reference wavelength for obtaining the technical characters.

The optical image capturing system could work in three visible light wavelengths, including 486.1 nm, 587.5 nm, and 656.2 nm, wherein 587.5 nm is the main reference wavelength and is the reference wavelength for obtaining the technical characters. The optical image capturing system can also work in five wavelengths, including 470 nm, 510 nm, 555 nm, 610 nm, and 650 nm wherein 555 nm is the main reference wavelength, and is the reference wavelength for obtaining the visible light technical characters.

The optical image capturing system of the present invention satisfies 0.5≤ΣPPR/|ΣNPR|≤15, and a preferable range is 1≤ΣPPR/|ΣNPR|≤3.0, where PPR is a ratio of the focal length f of the optical image capturing system to a focal length fp of each of lenses with positive refractive power; NPR is a ratio of the focal length f of the optical image capturing system to a focal length fn of each of lenses with negative refractive power; ΣPPR is a sum of the PPRs of each positive lens; and ΣNPR is a sum of the NPRs of each negative lens. It is helpful for control of an entire refractive power and an entire length of the optical image capturing system.

The image sensor is provided on the image plane, and is provided with at least one hundred thousand pixels. The optical image capturing system of the present invention satisfies HOS/HOI≤10 and 0.5≤HOS/f≤10, and a preferable range is 1≤HOS/HOI≤5 and 1≤HOS/f≤7, where HOI is a half of a diagonal of an effective sensing area of the image sensor, i.e., the maximum image height, and HOS is a height of the optical image capturing system, i.e. a distance on the optical axis between the object-side surface of the first lens and the image plane specifically for the infrared light. It is helpful for reduction of the size of the system for used in compact cameras.

The optical image capturing system of the present invention further is provided with an aperture to increase image quality.

In the optical image capturing system of the present invention, the aperture could be a front aperture or a middle aperture, wherein the front aperture is provided between the object and the first lens, and the middle is provided between the first lens and the image plane specifically for the infrared light. The front aperture provides a long distance between an exit pupil of the system and the image plane specifically for the infrared light, which allows more elements to be installed. The middle could enlarge a view angle of view of the system and increase the efficiency of the image sensor. The optical image capturing system satisfies 0.2≤InS/HOS≤1.1, where InS is a distance between the aperture and the image-side surface of the sixth lens. It is helpful for size reduction and wide angle.

The optical image capturing system of the present invention satisfies 0.1≤ΣTP/InTL≤0.9, where InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens, and ΣTP is a sum of central thicknesses of the lenses on the optical axis. It is helpful for the contrast of image and yield rate of manufacture and provides a suitable back focal length for installation of other elements.

The optical image capturing system of the present invention satisfies 0.001≤|R1/R2|≤20, and a preferable range is 0.01≤|R1/R2|≤10, where R1 is a radius of curvature of the object-side surface of the first lens, and R2 is a radius of curvature of the image-side surface of the first lens. It provides the first lens with a suitable positive refractive power to reduce the increase rate of the spherical aberration.

The optical image capturing system of the present invention satisfies −7<(R13−R14)/(R13+R14)<50, where R13 is a radius of curvature of the object-side surface of the seventh lens, and R14 is a radius of curvature of the image-side surface of the seventh lens. It may modify the astigmatic field curvature.

The optical image capturing system of the present invention satisfies IN12/f≤3.0, where IN12 is a distance on the optical axis between the first lens and the second lens. It may correct chromatic aberration and improve the performance.

The optical image capturing system of the present invention satisfies IN67/f≤0.8, where IN67 is a distance on the optical axis between the sixth lens and the seventh lens. It may correct chromatic aberration and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≤(TP1+IN12)/TP2≤10, where TP1 is a central thickness of the first lens on the optical axis, and TP2 is a central thickness of the second lens on the optical axis. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≤(TP7+IN67)/TP6≤10, where TP6 is a central thickness of the sixth lens on the optical axis, TP7 is a central thickness of the seventh lens on the optical axis, and IN67 is a distance between the sixth lens and the seventh lens. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≤TP4/(IN34+TP4+IN45)<1, where TP3 is a central thickness of the third lens on the optical axis, TP4 is a central thickness of the fourth lens on the optical axis, TP5 is a central thickness of the fifth lens on the optical axis, IN34 is a distance on the optical axis between the third lens and the fourth lens, IN45 is a distance on the optical axis between the fourth lens and the fifth lens, and InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens. It may fine tune and correct the aberration of the incident rays layer by layer, and reduce the height of the system.

The optical image capturing system satisfies 0 mm≤HVT71≤3 mm; 0 mm<HVT72≤6 mm; 0≤HVT71/HVT72; 0 mm≤|SGC71|≤0.5 mm; 0 mm<|SGC72|≤2 mm; and 0<|SGC72|/(|SGC72|+TP7)≤0.9, where HVT71 a distance perpendicular to the optical axis between the critical point C71 on the object-side surface of the seventh lens and the optical axis; HVT72 a distance perpendicular to the optical axis between the critical point C72 on the image-side surface of the seventh lens and the optical axis; SGC71 is a distance on the optical axis between a point on the object-side surface of the seventh lens where the optical axis passes through and a point where the critical point C71 projects on the optical axis; SGC72 is a distance on the optical axis between a point on the image-side surface of the seventh lens where the optical axis passes through and a point where the critical point C72 projects on the optical axis. It is helpful to correct the off-axis view field aberration.

The optical image capturing system satisfies 0.2≤HVT72/HOI≤0.9, and preferably satisfies 0.3≤HVT72/HOI≤0.8. It may help to correct the peripheral aberration.

The optical image capturing system satisfies 0≤HVT72/HOS≤0.5, and preferably satisfies 0.2≤HVT72/HOS≤0.45. It may help to correct the peripheral aberration.

The optical image capturing system of the present invention satisfies 0<SGI711/(SGI711+TP7)≤0.9; 0<SGI721/(SGI721+TP7)≤0.9, and it is preferable to satisfy 0.1≤SGI711/(SGI711+TP7)≤0.6; 0.1≤SGI721/(SGI721+TP7)≤0.6, where SGI711 is a displacement on the optical axis from a point on the object-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI721 is a displacement on the optical axis from a point on the image-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

The optical image capturing system of the present invention satisfies 0<SGI712/(SGI712+TP7)≤0.9; 0<SGI722/(SGI722+TP7)≤0.9, and it is preferable to satisfy 0.1≤SGI712/(SGI712+TP7)≤0.6; 0.1≤SGI722/(SGI722+TP7)≤0.6, where SGI712 is a displacement on the optical axis from a point on the object-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI722 is a displacement on the optical axis from a point on the image-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤|HIF711|≤5 mm; 0.001 mm≤|HIF721|≤5 mm, and it is preferable to satisfy 0.1 mm≤|HIF711|≤3.5 mm; 1.5 mm≤|HIF721|≤3.5 mm, where HIF711 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis; HIF721 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤|HIF712|≤5 mm; 0.001 mm≤|HIF722|≤5 mm, and it is preferable to satisfy 0.1 mm≤|HIF722|≤3.5 mm; 0.1 mm≤|HIF712|≤3.5 mm, where HIF712 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the second closest to the optical axis, and the optical axis; HIF722 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the second closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤|HIF713|≤5 mm; 0.001 mm≤|HIF723|≤5 mm, and it is preferable to satisfy 0.1 mm≤|HIF723|≤3.5 mm; 0.1 mm≤|HIF713|≤3.5 mm, where HIF713 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the third closest to the optical axis, and the optical axis; HIF723 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the third closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤|HIF714|≤5 mm; 0.001 mm≤|HIF724|≤5 mm, and it is preferable to satisfy 0.1 mm≤|HIF724|≤3.5 mm; 0.1 mm≤|HIF714|≤3.5 mm, where HIF714 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the fourth closest to the optical axis, and the optical axis; HIF724 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the fourth closest to the optical axis, and the optical axis.

In an embodiment, the lenses of high Abbe number and the lenses of low Abbe number are arranged in an interlaced arrangement that could be helpful for correction of aberration of the system.

An equation of aspheric surface is z=ch ²/[1+[1−(k+1)c ² h ²]^(0.5)]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹² +A14h ¹⁴ +A 16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+ . . .  (1)

where z is a depression of the aspheric surface; k is conic constant; c is reciprocal of the radius of curvature; and A4, A6, A8, A10, A12, A14, A16, A18, and A20 are high-order aspheric coefficients.

In the optical image capturing system, the lenses could be made of plastic or glass. The plastic lenses may reduce the weight and lower the cost of the system, and the glass lenses may control the thermal effect and enlarge the space for arrangement of the refractive power of the system. In addition, the opposite surfaces (object-side surface and image-side surface) of the first to the seventh lenses could be aspheric that can obtain more control parameters to reduce aberration. The number of aspheric glass lenses could be less than the conventional spherical glass lenses, which is helpful for reduction of the height of the system.

When the lens has a convex surface, which means that the surface is convex around a position, through which the optical axis passes, and when the lens has a concave surface, which means that the surface is concave around a position, through which the optical axis passes.

The optical image capturing system of the present invention could be applied in a dynamic focusing optical system. It is superior in the correction of aberration and high imaging quality so that it could be allied in lots of fields.

The optical image capturing system of the present invention could further include a driving module to meet different demands, wherein the driving module can be coupled with the lenses to move the lenses. The driving module can be a voice coil motor (VCM), which is used to move the lens for focusing, or can be an optical image stabilization (OIS) component, which is used to lower the possibility of having the problem of image blurring which is caused by subtle movements of the lens while shooting.

To meet different requirements, at least one lens among the first lens to the seventh lens of the optical image capturing system of the present invention can be a light filter, which filters out light of wavelength shorter than 500 nm. Such effect can be achieved by coating on at least one surface of the lens, or by using materials capable of filtering out short waves to make the lens.

To meet different requirements, the image plane specifically for the infrared light of the optical image capturing system in the present invention can be either flat or curved. If the image plane specifically for the infrared light is curved (e.g., a sphere with a radius of curvature), the incidence angle required for focusing light on the image plane specifically for the infrared light can be decreased, which is not only helpful to shorten the length of the system (TTL), but also helpful to increase the relative illuminance.

The optical image capturing system of the present invention could be applied to three-dimensional image capture. A light with specific characteristics is projected onto an object, and is reflected by a surface of the object, and is then received and calculated and analyzed by the lens to obtain the distance between each position of the object and the lens, thereby to determine the information of the three-dimensional image. The light projection usually uses infrared rays in a specific wavelength to reduce interference, thereby to achieving more accurate measurement. The detecting way for capturing the three-dimensional image could be, but not limited to, technologies such as time-of-flight (TOF) or structured light.

We provide several embodiments in conjunction with the accompanying drawings for the best understanding, which are:

First Embodiment

As shown in FIG. 1A and FIG. 1B, an optical image capturing system 10 of the first embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 110, a second lens 120, a third lens 130, an aperture 100, a fourth lens 140, a fifth lens 150, a sixth lens 160, a seventh lens 170, an infrared rays filter 180, an image plane 190 specifically for the infrared light, and an image sensor 192. FIG. 1C shows a modulation transformation of the optical image capturing system 10 of the first embodiment of the present application in infrared spectrum.

The first lens 110 has negative refractive power and is made of plastic. An object-side surface 112 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 114 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 112 has an inflection point, and the image-side surface 114 has two inflection points. A thickness of the first lens 110 on the optical axis is TP1, and a thickness of the first lens 110 at the height of a half of the entrance pupil diameter (HEP) is denoted by ETP1.

The first lens satisfies SGI111=−0.1110 mm; SGI121=2.7120 mm; TP1=2.2761 mm; |SGI111|/(|SGI111|+TP1)=0.0465; |SGI121|/(|SGI121|+TP1)=0.5437, where a displacement on the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis, is denoted by SGI111, and a displacement on the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis is denoted by SGI121.

The first lens satisfies SGI112=0 mm; SGI122=4.2315 mm; |SGI112|/(|SGI112|+TP1)=0; |SGI122|/(|SGI122|+TP1)=0.6502, where a displacement on the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the second closest to the optical axis, projects on the optical axis, is denoted by SGI112, and a displacement on the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the second closest to the optical axis, projects on the optical axis is denoted by SGI122.

The first lens satisfies HIF111=12.8432 mm; HIF111/HOI=1.7127; HIF121=7.1744 mm; HIF121/HOI=0.9567, where a displacement perpendicular to the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF111, and a displacement perpendicular to the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF121.

The first lens satisfies HIF112=0 mm; HIF112/HOI=0; HIF122=9.8592 mm; HIF122/HOI=1.3147, where a displacement perpendicular to the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the second closest to the optical axis is denoted by HIF112, and a displacement perpendicular to the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the second closest to the optical axis is denoted by HIF122.

The second lens 120 has positive refractive power and is made of plastic. An object-side surface 122 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 124 thereof, which faces the image side, is a concave aspheric surface. A thickness of the second lens 120 on the optical axis is TP2, and thickness of the second lens 120 at the height of a half of the entrance pupil diameter (HEP) is denoted by ETP2.

For the second lens, a displacement on the optical axis from a point on the object-side surface of the second lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis, is denoted by SGI211, and a displacement on the optical axis from a point on the image-side surface of the second lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis is denoted by SGI221.

For the second lens, a displacement perpendicular to the optical axis from a point on the object-side surface of the second lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF211, and a displacement perpendicular to the optical axis from a point on the image-side surface of the second lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF221.

The third lens 130 has negative refractive power and is made of plastic. An object-side surface 132, which faces the object side, is a convex aspheric surface, and an image-side surface 134, which faces the image side, is a concave aspheric surface. A thickness of the third lens 130 on the optical axis is TP3, and a thickness of the third lens 130 at the height of a half of the entrance pupil diameter (HEP) is denoted by ETP3.

For the third lens 130, SGI311 is a displacement on the optical axis from a point on the object-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI321 is a displacement on the optical axis from a point on the image-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

For the third lens 130, SGI312 is a displacement on the optical axis from a point on the object-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI322 is a displacement on the optical axis from a point on the image-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis.

For the third lens 130, HIF311 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens, which is the closest to the optical axis, and the optical axis; HIF321 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the third lens, which is the closest to the optical axis, and the optical axis.

For the third lens 130, HIF312 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens, which is the second closest to the optical axis, and the optical axis; HIF322 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the third lens, which is the second closest to the optical axis, and the optical axis.

The fourth lens 140 has positive refractive power and is made of plastic. An object-side surface 142, which faces the object side, is a convex aspheric surface, and an image-side surface 144, which faces the image side, is a convex aspheric surface. The object-side surface 142 has an inflection point. A thickness of the fourth lens 140 on the optical axis is TP4, and a thickness of the fourth lens 140 at the height of a half of the entrance pupil diameter (HEP) is denoted by ETP4.

The fourth lens 140 satisfies SGI411=0.0018 mm; |SGI411|/(|SGI411|+TP4)=0.0009, where SGI411 is a displacement on the optical axis from a point on the object-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI421 is a displacement on the optical axis from a point on the image-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

For the fourth lens 140, SGI412 is a displacement on the optical axis from a point on the object-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI422 is a displacement on the optical axis from a point on the image-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis.

The fourth lens 140 further satisfies HIF411=0.7191 mm; HIF411/HOI=0.0959, where HIF411 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens, which is the closest to the optical axis, and the optical axis; HIF421 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens, which is the closest to the optical axis, and the optical axis.

For the fourth lens 140, HIF412 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens, which is the second closest to the optical axis, and the optical axis; HIF422 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens, which is the second closest to the optical axis, and the optical axis.

The fifth lens 150 has positive refractive power and is made of plastic. An object-side surface 152, which faces the object side, is a concave aspheric surface, and an image-side surface 154, which faces the image side, is a convex aspheric surface. The object-side surface 152 and the image-side surface 154 both have an inflection point. A thickness of the fifth lens 150 on the optical axis is TP5, and a thickness of the fifth lens 150 at the height of a half of the entrance pupil diameter (HEP) is denoted by ETP5.

The fifth lens 150 satisfies SGI511=−0.1246 mm; SGI521=−2.1477 mm; |SGI511|/(|SGI511|+TP5)=0.0284; |SG1521|/(|SG1521|+TP5)=0.3346, where SGI511 is a displacement on the optical axis from a point on the object-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI521 is a displacement on the optical axis from a point on the image-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

For the fifth lens 150, SGI512 is a displacement on the optical axis from a point on the object-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI522 is a displacement on the optical axis from a point on the image-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis.

The fifth lens 150 further satisfies HIF511=3.8179 mm; HIF521=4.5480 mm; HIF511/HOI=0.5091; HIF521/HOI=0.6065, where HIF511 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fifth lens, which is the closest to the optical axis, and the optical axis; HIF521 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fifth lens, which is the closest to the optical axis, and the optical axis.

For the fifth lens 150, HIF512 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fifth lens, which is the second closest to the optical axis, and the optical axis; HIF522 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fifth lens, which is the second closest to the optical axis, and the optical axis.

The sixth lens 160 has negative refractive power and is made of plastic. An object-side surface 162, which faces the object side, is a convex aspheric surface, and an image-side surface 164, which faces the image side, is a concave aspheric surface. The object-side surface 162 and the image-side surface 164 both have an inflection point. Whereby, the incident angle of each view field entering the sixth lens 160 can be effectively adjusted to improve aberration. A thickness of the sixth lens 160 on the optical axis is TP6, and a thickness of the sixth lens 160 at the height of a half of the entrance pupil diameter (HEP) is denoted by ETP6.

The sixth lens 160 satisfies SGI611=0.3208 mm; SGI621=0.5937 mm; |SGI611|/(|SGI611|+TP6)=0.5167; |SGI621|/(|SGI621|+TP6)=0.6643, where SGI611 is a displacement on the optical axis from a point on the object-side surface of the sixth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI621 is a displacement on the optical axis from a point on the image-side surface of the sixth lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

The sixth lens 160 further satisfies HIF611=1.9655 mm; HIF621=2.0041 mm; HIF611/HOI=0.2621; HIF621/HOI=0.2672, where HIF611 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the sixth lens, which is the closest to the optical axis, and the optical axis; HIF621 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the sixth lens, which is the closest to the optical axis, and the optical axis.

The seventh lens 170 has positive refractive power and is made of plastic. An object-side surface 172, which faces the object side, is a convex aspheric surface, and an image-side surface 174, which faces the image side, is a concave aspheric surface. The object-side surface 172 and the image-side surface 174 both have an inflection point. A thickness of the seventh lens 170 on the optical axis is TP7, and a thickness of the seventh lens 170 at the height of a half of the entrance pupil diameter (HEP) is denoted by ETP7.

The seventh lens 170 satisfies SGI711=0.5212 mm; SGI721=0.5668 mm; |SGI711|/(|SGI711|+TP7)=0.3179; |SGI721|/(|SGI721|+TP7)=0.3364, where SGI711 is a displacement on the optical axis from a point on the object-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI721 is a displacement on the optical axis from a point on the image-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

The seventh lens 170 further satisfies HIF711=1.6707 mm; HIF721=1.8616 mm; HIF711/HOI=0.2228; HIF721/HOI=0.2482, where HIF711 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis; HIF721 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis.

A distance in parallel with the optical axis between a coordinate point at a height of ½ HEP on the object-side surface of the first lens 110 and the image plane specifically for the infrared light is ETL, and a distance in parallel with the optical axis between the coordinate point at the height of ½ HEP on the object-side surface of the first lens 110 and a coordinate point at a height of ½ HEP on the image-side surface of the seventh lens 140 is EIN, which satisfies: ETL=26.980 mm; EIN=24.999 mm; EIN/ETL=0.927.

The optical image capturing system of the first embodiment satisfies: ETP1=2.470 mm; ETP2=5.144 mm; ETP3=0.898 mm; ETP4=1.706 mm; ETP5=3.901 mm; ETP6=0.528 mm; ETP7=1.077 mm. The sum of the aforementioned ETP1 to ETP7 is SETP, wherein SETP=15.723 mm. In addition, TP1=2.276 mm; TP2=5.240 mm; TP3=0.837 mm; TP4=2.002 mm; TP5=4.271 mm; TP6=0.300 mm; TP7=1.118 mm. The sum of the aforementioned TP1 to TP7 is STP, wherein STP=16.044 mm. In addition, SETP/STP=0.980, and SETP/EIN=0.629.

In order to enhance the ability of correcting aberration and to lower the difficulty of manufacturing at the same time, the ratio between the thickness (ETP) at the height of a half of the entrance pupil diameter (HEP) and the thickness (TP) of any lens on the optical axis (i.e., ETP/TP) in the optical image capturing system of the first embodiment is particularly controlled, which satisfies: ETP1/TP1=1.085; ETP2/TP2=0.982; ETP3/TP3=1.073; ETP4/TP4=0.852; ETP5/TP5=0.914; ETP6/TP6=1.759; ETP7/TP7=0.963.

In order to enhance the ability of correcting aberration, lower the difficulty of manufacturing, and “slightly shortening” the length of the optical image capturing system at the same time, the ratio between the horizontal distance (ED) between two neighboring lenses at the height of a half of the entrance pupil diameter (HEP) and the parallel distance (IN) between these two neighboring lens on the optical axis (i.e., ED/IN) in the optical image capturing system of the first embodiment is particularly controlled, which satisfies: the horizontal distance between the first lens 110 and the second lens 120 at the height of a half of the entrance pupil diameter (HEP) is denoted by ED12, wherein ED12=4.474 mm; the horizontal distance between the second lens 120 and the third lens 130 at the height of a half of the entrance pupil diameter (HEP) is denoted by ED23, wherein ED23=0.349 mm; the horizontal distance between the third lens 130 and the fourth lens 140 at the height of a half of the entrance pupil diameter (HEP) is denoted by ED34, wherein ED34=1.660 mm; the horizontal distance between the fourth lens 140 and the fifth lens 150 at the height of a half of the entrance pupil diameter (HEP) is denoted by ED45, wherein ED45=1.794 mm; the horizontal distance between the fifth lens 150 and the sixth lens 160 at the height of a half of the entrance pupil diameter (HEP) is denoted by ED56, wherein ED56=0.714 mm; the horizontal distance between the sixth lens 160 and the seventh lens 170 at the height of a half of the entrance pupil diameter (HEP) is denoted by ED67, wherein ED67=0.284 mm. The sum of the aforementioned ED12 to ED67 is SED, wherein SED=9.276 mm.

The horizontal distance between the first lens 110 and the second lens 120 on the optical axis is denoted by IN12, wherein IN12=4.552 mm, and ED12/IN12=0.983. The horizontal distance between the second lens 120 and the third lens 130 on the optical axis is denoted by IN23, wherein IN23=0.162 mm, and ED23/IN23=2.153. The horizontal distance between the third lens 130 and the fourth lens 140 on the optical axis is denoted by IN34, wherein IN34=1.927 mm, and ED34/IN34=0.862. The horizontal distance between the fourth lens 140 and the fifth lens 150 on the optical axis is denoted by IN45, wherein IN45=1.515 mm, and ED45/IN45=1.184. The horizontal distance between the fifth lens 150 and the sixth lens 160 on the optical axis is denoted by IN56, wherein IN56=0.050 mm, and ED56/IN56=14.285. The horizontal distance between the sixth lens 160 and the seventh lens 170 on the optical axis is denoted by IN67, wherein IN67=0.211 mm, and ED67/IN67=1.345. The sum of the aforementioned IN12 to IN67 is denoted by SIN, wherein SIN=8.418, and SED/SIN=1.102.

The optical image capturing system of the first embodiment satisfies: ED12/ED23=12.816; ED23/ED34=0.210; ED34/ED45=0.925; ED45/ED56=2.512; ED56/ED67=2.512; IN12/IN23=28.080; IN23/IN34=0.084; IN34/IN45=1.272; IN45/IN56=30.305; IN56/IN67=0.236.

The horizontal distance in parallel with the optical axis between a coordinate point at the height of ½ HEP on the image-side surface of the seventh lens 170 and image plane specifically for the infrared light is denoted by EBL, wherein EBL=1.982 mm. The horizontal distance in parallel with the optical axis between the point on the image-side surface of the seventh lens 170 where the optical axis passes through and the image plane specifically for the infrared light is denoted by BL, wherein BL=2.517 mm. The optical image capturing system of the first embodiment satisfies: EBL/BL=0.7874. The horizontal distance in parallel with the optical axis between the coordinate point at the height of ½ HEP on the image-side surface of the seventh lens 170 and the infrared rays filter 180 is denoted by EIR, wherein EIR=0.865 mm. The horizontal distance in parallel with the optical axis between the point on the image-side surface of the seventh lens 170 where the optical axis passes through and the infrared rays filter 180 is denoted by PIR, wherein PIR=1.400 mm, and it satisfies: EIR/PIR=0.618.

The description below and the features related to inflection points are obtained based on main reference wavelength of 555 nm.

The infrared rays filter 180 is made of glass and between the seventh lens 170 and the image plane 190 specifically for the infrared light. The infrared rays filter 180 gives no contribution to the focal length of the system.

The optical image capturing system 10 of the first embodiment has the following parameters, which are f=4.3019 mm; f/HEP=1.2; HAF=59.9968 degrees; and tan(HAF)=1.7318, where f is a focal length of the system; HAF is a half of the maximum field angle; and HEP is an entrance pupil diameter.

The parameters of the lenses of the first embodiment are f1=−14.5286 mm; |f/f1|=0.2961; f7=8.2933; |f1|>f7; |f1/f7|=1.7519, where f1 is a focal length of the first lens 110; and f7 is a focal length of the seventh lens 170.

The first embodiment further satisfies |f2|+|f3|+|f4|+|f5|+|f6|=144.7494; |f1|+|f7|=22.8219 and |f2|+|f3|+|f4|+|f5|+|f6|>|f1|+|f7|, where f2 is a focal length of the second lens 120, f3 is a focal length of the third lens 130, f4 is a focal length of the fourth lens 140, f5 is a focal length of the fifth lens 150, f6 is a focal length of the sixth lens 160, and f7 is a focal length of the seventh lens 170.

The optical image capturing system 10 of the first embodiment further satisfies 93 PPR=f/f2+f/f4+f/f5+f/f7=1.7384; ΣNPR=f/f1+f/f3+f/f6=−0.9999; ΣPPR/|ΣNPR|=1.7386; |f/f2|=0.1774; |f/f3|=0.0443; |f/f4|=0.4411; |f/f5|=0.6012; |f/f6|=0.6595; |f/f7|=0.5187, where PPR is a ratio of a focal length f of the optical image capturing system to a focal length fp of each of the lenses with positive refractive power; and NPR is a ratio of a focal length f of the optical image capturing system to a focal length fn of each of lenses with negative refractive power.

The optical image capturing system 10 of the first embodiment further satisfies InTL+BFL=HOS; HOS=26.9789 mm; HOI=7.5 mm; HOS/HOI=3.5977; HOS/f=6.2715; InS=12.4615 mm; and InS/HOS=0.4619, where InTL is a distance between the object-side surface 112 of the first lens 110 and the image-side surface 174 of the seventh lens 170; HOS is a height of the image capturing system, i.e. a distance between the object-side surface 112 of the first lens 110 and the image plane specifically for the infrared light 190; InS is a distance between the aperture 100 and the image plane specifically for the infrared light 190; HOI is a half of a diagonal of an effective sensing area of the image sensor 192, i.e., the maximum image height; and BFL is a distance between the image-side surface 174 of the seventh lens 170 and the image plane specifically for the infrared light 190.

The optical image capturing system 10 of the first embodiment further satisfies ΣTP=16.0446 mm; and ΣTP/InTL=0.6559, where ΣTP is a sum of the thicknesses of the lenses 110-150 with refractive power. It is helpful for the contrast of image and yield rate of manufacture and provides a suitable back focal length for installation of other elements.

The optical image capturing system 10 of the first embodiment further satisfies |R1/R2|=129.9952, where R1 is a radius of curvature of the object-side surface 112 of the first lens 110, and R2 is a radius of curvature of the image-side surface 114 of the first lens 110. It provides the first lens with a suitable positive refractive power to reduce the increase rate of the spherical aberration.

The optical image capturing system 10 of the first embodiment further satisfies (R13-R14)/(R13+R14)=−0.0806, where R13 is a radius of curvature of the object-side surface 172 of the seventh lens 170, and R14 is a radius of curvature of the image-side surface 174 of the seventh lens 170. It may modify the astigmatic field curvature.

The optical image capturing system 10 of the first embodiment further satisfies 93 PP=f2+f4+f5+f7=49.4535 mm; and f4/(f2+f4+f5+f7)=0.1972, where ΣPP is a sum of the focal lengths fp of each lens with positive refractive power. It is helpful to share the positive refractive power of the fourth lens 140 to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment further satisfies ΣNP=f1+f3+f6=−118.1178 mm; and f1/(f1+f3+f6)=0.1677, where ΣNP is a sum of the focal lengths fn of each lens with negative refractive power. It is helpful to share the negative refractive power of the first lens 110 to the other negative lens, which avoid the significant aberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment further satisfies IN12=4.5524 mm; IN12/f=1.0582, where IN12 is a distance on the optical axis between the first lens 110 and the second lens 120. It may correct chromatic aberration and improve the performance.

The optical image capturing system 10 of the first embodiment further satisfies TP1=2.2761 mm; TP2=0.2398 mm; and (TP1+IN12)/TP2=1.3032, where TP1 is a central thickness of the first lens 110 on the optical axis, and TP2 is a central thickness of the second lens 120 on the optical axis. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system 10 of the first embodiment further satisfies TP6=0.3000 mm; TP7=1.1182 mm; and (TP7+IN67)/TP6=4.4322, where TP6 is a central thickness of the sixth lens 160 on the optical axis, TP7 is a central thickness of the seventh lens 170 on the optical axis, and IN67 is a distance on the optical axis between the sixth lens 160 and the seventh lens 170. It may control the sensitivity of manufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment further satisfies TP3=0.8369 mm; TP4=2.0022 mm; TP5=4.2706 mm; IN34=1.9268 mm; IN45=1.5153 mm; and TP4/(IN34+TP4+IN45)=0.3678, where TP3 is a central thickness of the third lens 130 on the optical axis, TP4 is a central thickness of the fourth lens 140 on the optical axis, TP5 is a central thickness of the fifth lens 150 on the optical axis; IN34 is a distance on the optical axis between the third lens 130 and the fourth lens 140; IN45 is a distance on the optical axis between the fourth lens 140 and the fifth lens 150; InTL is a distance between the object-side surface 112 of the first lens 110 and the image-side surface 174 of the seventh lens 170. It may control the sensitivity of manufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment further satisfies InRS61=−0.7823 mm; InRS62=−0.2166 mm; and |InRS62|/TP6=0.722, where InRS61 is a displacement from a point on the object-side surface 162 of the sixth lens 160 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the object-side surface 162 of the sixth lens 160 ends; InRS62 is a displacement from a point on the image-side surface 164 of the sixth lens 160 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the image-side surface 164 of the sixth lens 160 ends; and TP6 is a central thickness of the sixth lens 160 on the optical axis. It is helpful for manufacturing and shaping of the lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment further satisfies HVT61=3.3498 mm; HVT62=3.9860 mm; and HVT61/HVT62=0.8404, where HVT61 is a distance perpendicular to the optical axis between the critical point on the object-side surface 162 of the sixth lens 160 and the optical axis; and HVT62 is a distance perpendicular to the optical axis between the critical point on the image-side surface 164 of the sixth lens 160 and the optical axis.

The optical image capturing system 10 of the first embodiment further satisfies InRS71=−0.2756 mm; InRS72=−0.0938 mm; and |InRS72|/TP7=0.0839, where InRS71 is a displacement from a point on the object-side surface 172 of the seventh lens 170 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the object-side surface 172 of the seventh lens 170 ends; InRS72 is a displacement from a point on the image-side surface 174 of the seventh lens 170 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the image-side surface 174 of the seventh lens 170 ends; and TP7 is a central thickness of the seventh lens 170 on the optical axis. It is helpful for manufacturing and shaping of the lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment satisfies HVT71=3.6822 mm; HVT72=4.0606 mm; and HVT71/HVT72=0.9068, where HVT71 is a distance perpendicular to the optical axis between the critical point on the object-side surface 172 of the seventh lens 170 and the optical axis; and HVT72 is a distance perpendicular to the optical axis between the critical point on the image-side surface 174 of the seventh lens 170 and the optical axis.

The optical image capturing system 10 of the first embodiment satisfies HVT72/HOI=0.5414. It is helpful for correction of the aberration of the peripheral view field of the optical image capturing system.

The optical image capturing system 10 of the first embodiment satisfies HVT72/HOS=0.1505. It is helpful for correction of the aberration of the peripheral view field of the optical image capturing system.

The second lens 120, the third lens 130, and the seventh lens 170 have negative refractive power. The optical image capturing system 10 of the first embodiment further satisfies 1≤NA7/NA2, where NA2 is an Abbe number of the second lens 120; NA3 is an Abbe number of the third lens 130; and NA7 is an Abbe number of the seventh lens 170. It may correct the aberration of the optical image capturing system.

The optical image capturing system 10 of the first embodiment further satisfies |TDT|=2.5678%; |ODT|=2.1302%, where TDT is TV distortion; and ODT is optical distortion.

For the optical image capturing system of the first embodiment, the values of MTF in the spatial frequency of 55 cycles/mm at the optical axis, 0.3 field of view, and 0.7 field of view of visible light on an image plane specifically for the infrared light are respectively denoted by MTFE0, MTFE3, and MTFE7, wherein MTFE0 is around 0.35, MTFE3 is around 0.14, and MTEF7 is around 0.28; the values of MTF in the spatial frequency of 110 cycles/mm at the optical axis, 0.3 field of view, and 0.7 field of view of visible light on an image plane specifically for the infrared light are respectively denoted by MTFQ0, MTFQ3, and MTFQ7, wherein MTFQ0 is around 0.126, MTFQ3 is around 0.075, and MTFQ7 is around 0.177; the values of modulation transfer function (MTF) in the spatial frequency of 220 cycles/mm at the optical axis, 0.3 field of view, and 0.7 field of view on an image plane specifically for the infrared light are respectively denoted by MTFH0, MTFH3, and MTFH7, wherein MTFH0 is around 0.01, MTFH3 is around 0.01, and MTFH7 is around 0.01.

For the optical image capturing system of the first embodiment, when the infrared of wavelength of 850 nm focuses on the image plane specifically for the infrared light, the values of MTF in spatial frequency (55 cycles/mm) at the optical axis, 0.3 HOI, and 0.7 HOI on an image plane specifically for the infrared light are respectively denoted by MTFI0, MTFI3, and MTFI7, wherein MTFI0 is around 0.01, MTFI3 is around 0.01, and MTFI7 is around 0.01.

The parameters of the lenses of the first embodiment are listed in Table 1 and Table 2.

TABLE 1 f = 4.3019 mm; f/HEP = 1.2; HAF = 59.9968 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens −1079.499964 2.276 plastic 1.565 58.00 −14.53 2 8.304149657 4.552 3 2^(nd) lens 14.39130913 5.240 plastic 1.650 21.40 24.25 4 130.0869482 0.162 5 3^(rd) lens 8.167310118 0.837 plastic 1.650 21.40 −97.07 6 6.944477468 1.450 7 Aperture plane 0.477 8 4^(th) lens 121.5965254 2.002 plastic 1.565 58.00 9.75 9 −5.755749302 1.515 10 5^(th) lens −86.27705938 4.271 plastic 1.565 58.00 7.16 11 −3.942936258 0.050 12 6^(th) lens 4.867364751 0.300 plastic 1.650 21.40 −6.52 13 2.220604983 0.211 14 7^(th) lens 1.892510651 1.118 plastic 1.650 21.40 8.29 15 2.224128115 1.400 16 Infrared rays plane 0.200 BK_7 1.517 64.2 filter 17 plane 0.917 18 Image plane plane 0 specifically for infrared light Reference wavelength (d-line): 555 mm.

TABLE 2 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k 2.500000E+01 −4.711931E−01 1.531617E+00 −1.153034E+01  −2.915013E+00  4.886991E+00 −3.459463E+01 A4 5.236918E−06 −2.117558E−04 7.146736E−05 4.353586E−04 5.793768E−04 −3.756697E−04  −1.292614E−03 A6 −3.014384E−08  −1.838670E−06 2.334364E−06 1.400287E−05 2.112652E−04 3.901218E−04 −1.602381E−05 A8 −2.487400E−10   9.605910E−09 −7.479362E−08  −1.688929E−07  −1.344586E−05  −4.925422E−05  −8.452359E−06 A10 1.170000E−12 −8.256000E−11 1.701570E−09 3.829807E−08 1.000482E−06 4.139741E−06  7.243999E−07 A12 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 A14 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 Surface 9 10 11 12 13 14 15 k −7.549291E+00 −5.000000E+01  −1.740728E+00  −4.709650E+00 −4.509781E+00 −3.427137E+00 −3.215123E+00  A4 −5.583548E−03 1.240671E−04 6.467538E−04 −1.872317E−03 −8.967310E−04 −3.189453E−03 −2.815022E−03  A6  1.947110E−04 −4.949077E−05  −4.981838E−05  −1.523141E−05 −2.688331E−05 −1.058126E−05 1.884580E−05 A8 −1.486947E−05 2.088854E−06 9.129031E−07 −2.169414E−06 −8.324958E−07  1.760103E−06 −1.017223E−08  A10 −6.501246E−08 −1.438383E−08  7.108550E−09 −2.308304E−08 −6.184250E−09 −4.730294E−08 3.660000E−12 A12  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00 A14  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00

The detail parameters of the first embodiment are listed in Table 1, in which the unit of the radius of curvature, thickness, and focal length are millimeter, and surface 0-10 indicates the surfaces of all elements in the system in sequence from the object side to the image side. Table 2 is the list of coefficients of the aspheric surfaces, in which A1-A20 indicate the coefficients of aspheric surfaces from the first order to the twentieth order of each aspheric surface. The following embodiments have the similar diagrams and tables, which are the same as those of the first embodiment, so we do not describe it again.

Second Embodiment

As shown in FIG. 2A and FIG. 2B, an optical image capturing system 20 of the second embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 210, an aperture 200, a second lens 220, a third lens 230, a fourth lens 240, a fifth lens 250, a sixth lens 260, a seventh lens 270, an infrared rays filter 280, an image plane 290, and an image sensor 292. FIG. 2C shows a modulation transformation of the optical image capturing system 20 of the second embodiment of the present application in infrared spectrum.

The first lens 210 has positive refractive power and is made of plastic. An object-side surface 212 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 214 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 212 has an inflection point.

The second lens 220 has negative refractive power and is made of plastic. An object-side surface 222 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 224 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 222 and the image-side surface 224 both have an inflection point.

The third lens 230 has positive refractive power and is made of plastic. An object-side surface 232, which faces the object side, is a convex aspheric surface, and an image-side surface 234, which faces the image side, is a concave aspheric surface. The image-side surface 234 has an inflection point.

The fourth lens 240 has positive refractive power and is made of plastic. An object-side surface 242, which faces the object side, is a convex aspheric surface, and an image-side surface 244, which faces the image side, is a concave aspheric surface. The object-side surface 242 has an inflection point, and the image-side surface 244 has an inflection point.

The fifth lens 250 has positive refractive power and is made of plastic. An object-side surface 252, which faces the object side, is a convex aspheric surface, and an image-side surface 254, which faces the image side, is a concave aspheric surface. The object-side surface 252 has an inflection point, and the image-side surface 254 has two inflection points.

The sixth lens 260 has positive refractive power and is made of plastic. An object-side surface 262, which faces the object side, is a convex aspheric surface, and an image-side surface 264, which faces the image side, is a concave aspheric surface. The object-side surface 262 has two inflection points, and the image-side surface 264 has two inflection points. Whereby, the incident angle of each view field entering the sixth lens 260 can be effectively adjusted to improve aberration.

The seventh lens 270 has negative refractive power and is made of plastic. An object-side surface 272, which faces the object side, is a concave aspheric surface, and an image-side surface 274, which faces the image side, is a concave aspheric surface. It may help to shorten the back focal length to keep small in size. In addition, the object-side surface 272 and the image-side surface 274 both have an inflection point, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 280 is made of glass and between the seventh lens 270 and the image plane specifically for the infrared light 290. The infrared rays filter 280 gives no contribution to the focal length of the system.

The parameters of the lenses of the second embodiment are listed in Table 3 and Table 4.

TABLE 3 f = 8.6556 mm; f/HEP = 1.4; HAF = 20.5346 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 3.608758597 1.959 plastic 1.544 56.09 8.454 2 13.8060016 0.490 3 Aperture 1E+18 0.150 4 2^(nd) lens −10.34008735 0.400 plastic 1.515 56.55 −9.136 5 8.654799118 0.050 6 3^(rd) lens 4.039776435 0.436 plastic 1.661 20.39 22.206 7 5.362440883 0.050 8 4^(th) lens 2.914317723 0.473 plastic 1.5441 56.090 9091.860 9 2.749936463 0.352 10 5^(th) lens 2.873983403 0.533 plastic 1.661 20.39 13.208 11 3.995948109 1.154 12 6^(th) lens 17.9817901 0.417 plastic 1.661 20.39 100.229 13 24.57331161 1.209 14 7^(th) lens −29.18117929 0.542 plastic 1.636 23.89 −9.731 15 7.792296656 0.171 16 Infrared rays 1E+18 0.215 BK_7 1.517 64.2 filter 17 1E+18 0.999 18 Image plane 1E+18 0.001 specifically for infrared light Reference wavelength: 940 nm; the position of blocking light: the effective half diameter of the clear aperture of the first surface is 3.437 mm; the effective half diameter of the clear aperture of the fifth surface is 2.950 mm; the effective half diameter of the clear aperture of the fifteenth surface is 2.970 mm; in the current embodiment, the first aperture is used for calculating the aperture value, and the exit pupil diameter of the image-side surface of the seventh lens is used as HXP

TABLE 4 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −6.020435E−01 −3.021045E+00 −3.926596E+01 −2.205177E+01 −1.813067E+00  2.043846E+00 −1.299930E+00  A4 −1.665998E−04 −2.865732E−03 −4.016547E−03 −2.327750E−03  1.086065E−02  1.594973E−02 4.428747E−03 A6  3.563534E−05  8.727019E−04  4.675536E−03  1.503727E−03 −1.841949E−03 −1.722523E−03 5.600680E−05 A8  1.472237E−05 −1.534967E−04 −1.124443E−03 −2.608390E−04 −3.422804E−04 −2.442256E−03 −9.417032E−04  A10 −5.304019E−06  2.881569E−05  1.769086E−04  1.070410E−05  1.340704E−04  9.160450E−04 1.480627E−04 A12  7.575763E−07 −3.136218E−06 −1.779748E−05  8.843343E−07 −1.534288E−05 −1.379784E−04 2.859123E−06 A14 −4.909059E−08  1.537957E−07  1.011806E−06 −5.694768E−08  6.102273E−07  9.285353E−06 −2.687307E−06  A16  1.080216E−09 −2.772807E−09 −2.452775E−08 −4.585678E−10  2.334429E−09 −2.244288E−07 1.820267E−07 Surface 9 10 11 12 13 14 15 k −3.444200E+00  −5.441012E+00  2.299813E−01 −8.999827E+01 −3.396539E+01  8.999091E+01 −2.361751E+01 A4 4.716089E−03 8.913614E−03 −1.707338E−02   1.419255E−03 −5.810072E−03 −4.010619E−02 −3.472495E−02 A6 5.746184E−04 −5.502425E−03  1.850544E−03 −6.280987E−03 −3.099095E−04  8.903957E−03  7.861744E−03 A8 4.056198E−05 3.956161E−04 −1.963177E−03   3.301723E−03  3.772465E−05 −2.222118E−03 −1.724419E−03 A10 −4.277343E−04  2.175856E−04 7.910576E−04 −1.513522E−03 −3.210133E−05  6.986359E−04  3.179609E−04 A12 1.254760E−04 −4.394603E−05  −1.177970E−04   4.042532E−04  1.202548E−05 −1.361232E−04 −3.865119E−05 A14 −1.438544E−05  1.726265E−06 3.472448E−06 −5.898805E−05 −3.410486E−06  1.263136E−05  2.473662E−06 A16 6.053910E−07 6.027942E−08 3.380357E−07  3.479231E−06  3.016620E−07 −4.356463E−07 −6.225282E−08

An equation of the aspheric surfaces of the second embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the second embodiment based on Table 3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 940 nm) MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.88  0.67  0.52  0.74  0.38  0.39  ETP1 ETP2 ETP3 ETP4 ETP5 ETP6 1.444 0.539 0.522 0.303 0.598 0.638 ETP7 ETL EBL EIN EIR PIR 0.827 8.938 1.616 7.321 0.401 0.171 EIN/ETL SETP/EIN EIR/PIR SETP STP SETP/STP 0.819 0.665 2.352 4.871 4.760 1.023 ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.737 1.347 1.195 0.641 1.122 1.530 ETP7/TP7 BL EBL/BL SED SIN SED/SIN 1.526 1.214  1.3311 2.450 3.456 0.709 ED12 ED23 ED34 ED45 ED56 ED67 0.491 0.327 0.224 0.211 0.206 0.991 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56 ED67/IN67 0.766 6.546 4.480 0.601 0.178 0.820 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6|  1.0238  0.9475  0.3898  0.0010  0.6553  0.0864 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f  0.8895  1.5009  2.4923  0.6022  0.0740  0.1397 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6  0.9254  0.4114 6.4988 4.1996 HOS InTL HOS/HOI InS/HOS ODT % TDT %  9.4296  8.2157  2.8574  0.7403  1.7716  1.1496 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0    0     1.4874 0    0    0    HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS  0.7614  0.7282 0     0.8546  0.2590  0.0906 IN12 IN23 IN34 IN45 IN56 IN67 0.6405 mm 0.0500 mm 0.0500 mm 0.3520 mm 1.1540 mm 1.2092 mm

The results of the equations of the second embodiment based on Table 3 and Table 4 are listed in the following table:

Values related to the inflection points of the second embodiment (Reference wavelength: 940 nm) HIF111 2.7553 HIF111/HOI 0.8349 SGI111 1.0894 |SGI111|/(|SGI111| + TP1) 0.3574 HIF211 0.8718 HIF211/HOI 0.2642 SGI211 −0.0319 |SGI211|/(|SGI211| + TP2) 0.0739 HIF221 2.3452 HIF221/HOI 0.7107 SGI221 0.1573 |SGI221|/(|SGI221| + TP2) 0.2823 HIF321 2.3097 HIF321/HOI 0.6999 SGI321 0.5850 |SGI321|/(|SGI321| + TP3) 0.5727 HIF411 2.1383 HIF411/HOI 0.6480 SGI411 0.6674 |SGI411|/(|SGI411| + TP4) 0.5854 HIF421 1.3945 HIF421/HOI 0.4226 SGI421 0.2998 |SGI421|/(|SGI421| + TP4) 0.3881 HIF511 1.2786 HIF511/HOI 0.3875 SGI511 0.2374 |SGI511|/(|SGI511| + TP5) 0.3081 HIF521 1.4821 HIF521/HOI 0.4491 SGI521 0.2273 |SGI521|/(|SGI521| + TP5) 0.2989 HIF522 1.7387 HIF522/HOI 0.5269 SGI522 0.2907 |SGI522|/(|SGI522| + TP5) 0.3529 HIF611 0.4426 HIF611/HOI 0.1341 SGI611 0.0046 |SGI611|/(|SGI611| + TP6) 0.0109 HIF612 2.1144 HIF612/HOI 0.6407 SGI612 −0.4722 |SGI612|/(|SGI612| + TP6) 0.5311 HIF621 0.4180 HIF621/HOI 0.1267 SGI621 0.0030 |SGI621|/(|SGI621| + TP6) 0.0071 HIF622 2.2740 HIF622/HOI 0.6891 SGI622 −0.3952 |SGI622|/(|SGI622| + TP6) 0.4866 HIF711 2.5009 HIF711/HOI 0.7578 SGI711 −0.7984 |SGI711|/(|SGI711| + TP7) 0.5957 HIF721 0.4574 HIF721/HOI 0.1386 SGI721 0.0110 |SGI721|/(|SGI721| + TP7) 0.0198

Third Embodiment

As shown in FIG. 3A and FIG. 3B, an optical image capturing system 30 of the third embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 310, an aperture 300, a second lens 320, a third lens 330, a fourth lens 340, a fifth lens 350, a sixth lens 360, a seventh lens 370, an infrared rays filter 380, an image plane 390, and an image sensor 392. FIG. 3C shows a modulation transformation of the optical image capturing system 30 of the third embodiment of the present application in infrared spectrum.

The first lens 310 has positive refractive power and is made of plastic. An object-side surface 312 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 314 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 312 and the image-side surface 314 both have an inflection point.

The second lens 320 has negative refractive power and is made of plastic. An object-side surface 322 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 324 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 322 has two inflection points, and the image-side surface 324 has an inflection point.

The third lens 330 has positive refractive power and is made of plastic. An object-side surface 332 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 334 thereof, which faces the image side, is a concave aspheric surface.

The fourth lens 340 has negative refractive power and is made of plastic. An object-side surface 342, which faces the object side, is a convex aspheric surface, and an image-side surface 344, which faces the image side, is a concave aspheric surface. The object-side surface 342 has two inflection points, and the image-side surface 344 has an inflection point.

The fifth lens 350 has positive refractive power and is made of plastic. An object-side surface 352, which faces the object side, is a convex aspheric surface, and an image-side surface 354, which faces the image side, is a concave aspheric surface. The object-side surface 352 has three inflection points, and the image-side surface 354 has two inflection points.

The sixth lens 360 has positive refractive power and is made of plastic. An object-side surface 362, which faces the object side, is a convex aspheric surface, and an image-side surface 364, which faces the image side, is a convex aspheric surface. The object-side surface 362 has two inflection points, and the image-side surface 364 has an inflection point. Whereby, the incident angle of each view field entering the sixth lens 360 can be effectively adjusted to improve aberration.

The seventh lens 370 has negative refractive power and is made of plastic. An object-side surface 372, which faces the object side, is a convex aspheric surface, and an image-side surface 374, which faces the image side, is a concave aspheric surface. It may help to shorten the back focal length to keep small in size. In addition, the object-side surface 372 has two inflection points, and the image-side surface 374 has an inflection point, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 380 is made of glass and between the seventh lens 370 and the image plane 390 specifically for the infrared light. The infrared rays filter 380 gives no contribution to the focal length of the system.

The parameters of the lenses of the third embodiment are listed in Table 5 and Table 6.

TABLE 5 f = 8.6158 mm; f/HEP = 1.0; HAF = 20.5502 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 5.112456695 2.000 plastic 1.544 56.09 11.506 2 24.59945941 0.346 3 Aperture 1E+18 0.150 4 2^(nd) lens −12.29966691 0.419 plastic 1.515 56.55 −9.682 5 8.401305303 0.050 6 3^(rd) lens 3.380404133 1.347 plastic 1.661 20.39 10.088 7 5.855969919 0.431 8 4^(th) lens 2.7783257 0.543 plastic 1.544 56.09 −191.577 9 2.519978139 1.142 10 5^(th) lens 3.788193622 0.589 plastic 1.661 20.39 15.450 11 5.695684242 1.349 12 6^(th) lens 45.78926584 0.559 plastic 1.661 20.39 54.188 13 −154.4855046 0.230 14 7^(th) lens 4.700764222 0.394 plastic 1.636 23.89 −10.905 15 2.698147892 0.239 16 Infrared rays 1E+18 0.215 BK_7 1.517 64.2 filter 17 1E+18 0.999 18 Image plane 1E+18 0.001 specifically for infrared light Reference wavelength: 940 nm; the position of blocking light: the effective half diameter of the clear aperture of the fourth surface is 4.465 mm; the effective half diameter of the clear aperture of the fifth surface is 4.465 mm; the effective half diameter of the clear aperture of the ninth surface is 3.100 mm; the exit pupil diameter of the image-side surface of the seventh lens is used as HXP

TABLE 6 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −8.274930E−01 −2.567073E+01 −2.693232E+01 −2.822341E+00 −1.506280E+00  1.723385E+00 −1.229266E+00 A4 −5.472769E−04 −2.776560E−03  1.509562E−02  2.097049E−02  8.419929E−03  7.815428E−03 −3.376133E−03 A6  8.353616E−05  1.067811E−03 −2.074464E−03 −5.357177E−03 −2.037358E−03 −1.131033E−03  8.600724E−04 A8 −1.765267E−05 −1.776985E−04  1.840679E−04  5.811635E−04  3.306483E−04 −1.530358E−05 −4.592307E−04 A10  1.850435E−06  1.538122E−05 −1.186089E−05 −3.466600E−05 −5.206337E−05 −5.932071E−06  4.425298E−05 A12 −1.504192E−07 −7.429141E−07  6.368232E−07  1.172483E−06  5.742477E−06  3.389440E−06  1.538306E−06 A14  6.015457E−09  1.898004E−08 −2.219552E−08 −2.123347E−08 −3.343524E−07 −3.639285E−07 −4.269123E−07 A16 −8.820639E−11 −2.015608E−10  3.182121E−10  1.630629E−10  7.739030E−09  1.210206E−08  1.699109E−08 Surface 9 10 11 12 13 14 15 k −3.170098E+00 −7.290405E+00  4.256323E−01 −7.269228E+01 −3.156745E+01 −3.417011E+01 −1.398615E+01 A4  2.106319E−03  3.884817E−03 −1.052475E−02  1.455030E−02 −2.140274E−02 −1.349309E−01 −7.874989E−02 A6  1.472733E−03 −1.384577E−04  2.067012E−03 −2.247441E−02  5.048437E−03  5.903182E−02  3.133721E−02 A8 −9.134375E−04 −1.498622E−03 −1.797602E−03  1.365764E−02  2.037305E−03 −1.392772E−02 −7.652589E−03 A10  1.709433E−04  6.267565E−04  6.188574E−04 −5.233465E−03 −1.529550E−03  1.866830E−03  1.132295E−03 A12 −1.749428E−05 −1.281974E−04 −1.107698E−04  1.091974E−03  3.350093E−04 −1.454527E−04 −1.002298E−04 A14  9.481144E−07  1.283923E−05  9.987438E−06 −1.155219E−04 −3.278021E−05  6.348745E−06  4.896584E−06 A16 −2.050334E−08 −4.921486E−07 −3.343660E−07  4.839359E−06  1.227615E−06 −1.234321E−07 −1.019593E−07

An equation of the aspheric surfaces of the third embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the third embodiment based on Table 5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 940 nm) MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.81  0.77  0.44  0.53  0.54  0.26  ETP1 ETP2 ETP3 ETP4 ETP5 ETP6 1.429 0.844 1.039 0.506 0.499 0.761 ETP7 ETL EBL EIN EIR PIR 0.842 10.303  1.731 8.572 0.516 0.239 EIN/ETL SETP/EIN EIR/PIR SETP STP SETP/STP 0.832 0.691 2.162 5.919 5.850 1.012 ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.714 2.014 0.771 0.932 0.847 1.362 ETP7/TP7 BL EBL/BL SED SIN SED/SIN 2.138 1.259  1.37499 2.653 3.698 0.717 ED12 ED23 ED34 ED45 ED56 ED67 0.481 0.597 0.570 0.598 0.158 0.248 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56 ED67/IN67 0.969 11.948  1.325 0.524 0.117 1.077 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6|  0.7488  0.8899  0.8541  0.0450  0.5576  0.1590 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f  0.7901  1.8069  2.2376  0.8075  0.0576  0.0267 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6  1.1884  0.9598 5.9590 1.1168 HOS InTL HOS/HOI InS/HOS ODT % TDT % 10.8072  9.5482  3.2749  0.7829  2.1571  1.1847 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0     3.9133  1.2870 0    0    0    HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS  1.1503 0     0.6371  1.1627  0.3523  0.1076 IN12 IN23 IN34 IN45 IN56 IN67 0.4963 mm 0.0500 mm 0.4306 mm 1.1416 mm 1.3492 mm 0.2301 mm

The results of the equations of the third embodiment based on Table 5 and Table 6 are listed in the following table:

Values related to the inflection points of the third embodiment (Reference wavelength: 940 nm) HIF111 3.1047 HIF111/HOI 0.9408 SGI111 0.9030 |SGI111|/(|SGI111| + TP1) 0.3111 HIF121 2.5770 HIF121/HOI 0.7809 SGI121 0.1166 |SGI121|/(|SGI121| + TP1) 0.0551 HIF211 0.6855 HIF211/HOI 0.2077 SGI211 −0.0156 |SGI211|/(|SGI211| + TP2) 0.0359 HIF212 4.0370 HIF212/HOI 1.2233 SGI212 0.6671 |SGI212|/(|SGI212| + TP2) 0.6143 HIF221 1.9144 HIF221/HOI 0.5801 SGI221 0.3157 |SGI221|/(|SGI221| + TP2) 0.4298 HIF411 1.8240 HIF411/HOI 0.5527 SGI411 0.5411 |SGI411|/(|SGI411| + TP4) 0.4990 HIF412 3.1784 HIF412/HOI 0.9631 SGI412 1.0084 |SGI412|/(|SGI412| + TP4) 0.6498 HIF421 1.7809 HIF421/HOI 0.5397 SGI421 0.5307 |SGI421|/(|SGI421| + TP4) 0.4941 HIF511 1.4214 HIF511/HOI 0.4307 SGI511 0.2285 |SGI511|/(|SGI511| + TP5) 0.2795 HIF512 2.6242 HIF512/HOI 0.7952 SGI512 0.3486 |SGI512|/(|SGI512| + TP5) 0.3717 HIF513 2.7118 HIF513/HOI 0.8218 SGI513 0.3353 |SGI513|/(|SGI513| + TP5) 0.3627 HIF521 1.2111 HIF521/HOI 0.3670 SGI521 0.1097 |SGI521|/(|SGI521| + TP5) 0.1570 HIF522 2.2993 HIF522/HOI 0.6968 SGI522 0.1878 |SGI522|/(|SGI522| + TP5) 0.2418 HIF611 0.7630 HIF611/HOI 0.2312 SGI611 0.0081 |SGI611|/(|SGI611| + TP6) 0.0143 HIF612 2.5897 HIF612/HOI 0.7848 SGI612 −0.7611 |SGI612|/(|SGI612| + TP6) 0.5767 HIF621 2.7384 HIF621/HOI 0.8298 SGI621 −0.7906 |SGI621|/(|SGI621| + TP6) 0.5859 HIF711 0.3426 HIF711/HOI 0.1038 SGI711 0.0102 |SGI711|/(|SGI711| + TP7) 0.0253 HIF712 2.5914 HIF712/HOI 0.7853 SGI712 −0.6472 |SGI712|/(|SGI712| + TP7) 0.6217 HIF721 0.5314 HIF721/HOI 0.1610 SGI721 0.0414 |SGI721|/(|SGI721| + TP7) 0.0951

Fourth Embodiment

As shown in FIG. 4A and FIG. 4B, an optical image capturing system 40 of the fourth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 410, an aperture 400, a second lens 420, a third lens 430, a fourth lens 440, a fifth lens 450, a sixth lens 460, a seventh lens 470, an infrared rays filter 480, an image plane 490 specifically for the infrared light, and an image sensor 492. FIG. 4C shows a modulation transformation of the optical image capturing system 40 of the fourth embodiment of the present application in infrared spectrum.

The first lens 410 has positive refractive power and is made of plastic. An object-side surface 412 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 414 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 412 has an inflection point.

The second lens 420 has negative refractive power and is made of plastic. An object-side surface 422 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 424 thereof, which faces the image side, is a concave aspheric surface. The image-side surface 424 has an inflection point.

The third lens 430 has positive refractive power and is made of plastic. An object-side surface 432 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 434 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 432 has two inflection points, and the image-side surface 434 has three inflection points.

The fourth lens 440 has positive refractive power and is made of plastic. An object-side surface 442, which faces the object side, is a convex aspheric surface, and an image-side surface 444, which faces the image side, is a concave aspheric surface. The object-side surface 442 and the image-side surface 444 both have two inflection points.

The fifth lens 450 has positive refractive power and is made of plastic. An object-side surface 452, which faces the object side, is a convex aspheric surface, and an image-side surface 454, which faces the image side, is a concave aspheric surface. The object-side surface 452 has an inflection point, and the image-side surface 454 has an inflection point.

The sixth lens 460 has positive refractive power and is made of plastic. An object-side surface 462, which faces the object side, is a convex aspheric surface, and an image-side surface 464, which faces the image side, is a convex aspheric surface. The object-side surface 462 and the image-side surface 464 both have an inflection point. Whereby, the incident angle of each view field entering the sixth lens 460 can be effectively adjusted to improve aberration.

The seventh lens 470 has negative refractive power and is made of plastic. An object-side surface 472, which faces the object side, is a convex aspheric surface, and an image-side surface 474, which faces the image side, is a concave aspheric surface. The object-side surface 472 has two inflection points, and the image-side surface 474 has two inflection points. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 480 is made of glass and between the seventh lens 470 and the image plane 490 specifically for the infrared light. The infrared rays filter 480 gives no contribution to the focal length of the system.

The parameters of the lenses of the fourth embodiment are listed in Table 7 and Table 8.

TABLE 7 f = 6.7787 mm; f/HEP = 1.4; HAF = 25.6275 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 3.422929224 0.696 plastic 1.584 29.89 19.272 2 4.57054616 0.846 3 Aperture 1E+18 −0.321  4 2^(nd) lens 22.29252636 0.738 plastic 1.515 56.55 −35.085 5 9.836765156 0.150 6 3^(rd) lens 22.8180854 0.543 plastic 1.661 20.39 111.489 7 32.93339546 0.050 8 4^(th) lens 2.368073586 0.978 plastic 1.544 56.09 21.288 9 2.547918656 0.228 10 5^(th) lens 2.560253873 0.602 plastic 1.661 20.39 13.392 11 3.284885133 1.203 12 6^(th) lens 19.58525893 0.727 plastic 1.661 20.39 9.242 13 −8.586539162 0.758 14 7^(th) lens 29.10157108 0.359 plastic 1.636 23.89 −5.979 15 3.312112442 0.228 16 Infrared rays 1E+18 0.215 BK_7 1.517 64.2 filter 17 1E+18 1.000 18 Image plane 1E+18 0.000 specifically for infrared light Reference wavelength: 940 nm; the position of blocking light: the effective half diameter of the clear aperture of the sixth surface is 2.746 mm; the effective half diameter of the clear aperture of the seventh surface is 2.770 mm; the effective half diameter of the clear aperture of the fifteenth surface is 2.950 mm; the exit pupil diameter of the image-side surface of the seventh lens is used as HXP

TABLE 8 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −2.319837E+00 −9.200961E+00 6.852471E+01 −8.945487E+01 6.503287E+01 8.988503E+01 −1.212746E+00 A4  3.754323E−03  1.273511E−02 1.395197E−02  1.788787E−02 6.017742E−03 5.627701E−03 −7.360646E−04 A6 −1.816684E−03 −6.074251E−03 −9.687121E−03  −1.849369E−02 −3.743121E−03  −2.242977E−03  −2.492451E−03 A8  3.151676E−04  1.128158E−03 3.357512E−03  7.075838E−03 1.191534E−04 2.946467E−04  5.238502E−04 A10 −9.255319E−05 −1.091122E−04 −5.754096E−04  −1.482386E−03 3.004769E−04 7.993898E−06  9.690364E−05 A12  1.427989E−05  1.405535E−05 6.353942E−05  1.865340E−04 −8.628215E−05  −1.100013E−05  −8.752066E−05 A14 −8.699769E−07 −2.283839E−06 −5.080905E−06  −1.397226E−05 9.987259E−06 2.012662E−06  1.713495E−05 A16  1.727348E−08  1.565328E−07 2.010750E−07  4.914979E−07 −4.295077E−07  −1.254936E−07  −1.076750E−06 Surface 9 10 11 12 13 14 15 k −6.934912E+00 −6.306659E+00  2.138094E−01 −8.998695E+01 −2.749949E+01  8.900696E+01 −1.427832E+01 A4  6.565919E−03  1.977947E−03 −1.376303E−02 −3.332985E−03 −8.580272E−03 −1.087960E−01 −6.615250E−02 A6 −3.199442E−03 −1.176738E−03  5.012094E−03 −1.448698E−03  1.930532E−03  4.370249E−02  2.569579E−02 A8 −2.316685E−03 −2.220488E−03 −2.380857E−03  3.294246E−04 −2.070344E−04 −1.150533E−02 −6.706569E−03 A10  1.287927E−03  1.517894E−03  1.422015E−03  5.389812E−07 −8.202646E−07  2.030953E−03  1.138817E−03 A12 −2.686568E−04 −3.501910E−04 −3.495731E−04 −1.751515E−05  2.236784E−05 −2.179917E−04 −1.211066E−04 A14  2.893757E−05  3.727091E−05  3.396473E−05  2.739816E−06 −6.292785E−06  1.281568E−05  7.307362E−06 A16 −1.344272E−06 −1.680183E−06 −1.190062E−06 −3.335559E−07  4.770092E−07 −3.191279E−07 −1.887382E−07

An equation of the aspheric surfaces of the fourth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the fourth embodiment based on Table 7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 940 nm) MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.87  0.8  0.77  0.73  0.54  0.52  ETP1 ETP2 ETP3 ETP4 ETP5 ETP6 0.538 0.580 0.538 0.586 0.838 0.581 ETP7 ETL EBL EIN EIR PIR 0.830 8.420 1.495 6.925 0.280 0.228 EIN/ETL SETP/EIN EIR/PIR SETP STP SETP/STP 0.822 0.648 1.228 4.490 4.643 0.967 ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.773 0.786 0.992 0.598 1.391 0.799 ETP7/TP7 BL EBL/BL SED SIN SED/SIN 2.311 1.301  1.1491 2.435 2.914 0.836 ED12 ED23 ED34 ED45 ED56 ED67 0.353 0.153 0.810 0.405 0.205 0.510 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56 ED67/IN67 0.672 1.022 16.206  1.772 0.170 0.673 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6|  0.3517  0.1932  0.0608  0.3184  0.5062  0.7334 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f  1.1337  1.4644  1.8331  0.7989  0.0774  0.1118 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6  0.5493  0.3147 1.6544 1.5370 HOS InTL HOS/HOI InS/HOS ODT % TDT %  8.8584  7.5569  2.6844  0.8259  1.4828  0.5507 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0    0    0     2.1143 0    0    HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS  1.3795 0     0.2888  1.2077  0.3660  0.1363 IN12 IN23 IN34 IN45 IN56 IN67 0.5246 mm 0.1500 mm 0.0500 mm 0.2283 mm 1.2028 mm 0.7580 mm

The results of the equations of the fourth embodiment based on Table 7 and Table 8 are listed in the following table:

Values related to the inflection points of the fourth embodiment (Reference wavelength: 940 nm) HIF111 1.7103 HIF111/HOI 0.5183 SGI111 0.3943 |SGI111|/(|SGI111| + TP1) 0.3615 HIF112 2.5197 HIF112/HOI 0.7635 SGI112 0.6659 |SGI112|/(|SGI112| + TP1) 0.4888 HIF221 0.9477 HIF221/HOI 0.2872 SGI221 0.0437 |SGI221|/(|SGI221| + TP2) 0.0559 HIF311 1.2856 HIF311/HOI 0.3896 SGI311 0.0410 |SGI311|/(|SGI311| + TP3) 0.0703 HIF312 1.7426 HIF312/HOI 0.5281 SGI312 0.0660 |SGI312|/(|SGI312| + TP3) 0.1085 HIF321 1.6634 HIF321/HOI 0.5040 SGI321 0.0560 |SGI321|/(|SGI321| + TP3) 0.0936 HIF322 1.9304 HIF322/HOI 0.5850 SGI322 0.0725 |SGI322|/(|SGI322| + TP3) 0.1178 HIF323 2.4141 HIF323/HOI 0.7315 SGI323 0.1055 |SGI323|/(|SGI323| + TP3) 0.1629 HIF411 1.8227 HIF411/HOI 0.5523 SGI411 0.6271 |SGI411|/(|SGI411| + TP4) 0.3906 HIF421 1.1389 HIF421/HOI 0.3451 SGI421 0.2065 |SGI421|/(|SGI421| + TP4) 0.1743 HIF422 1.9022 HIF422/HOI 0.5764 SGI422 0.3904 |SGI422|/(|SGI422| + TP4) 0.2852 HIF511 2.1362 HIF511/HOI 0.6473 SGI511 0.5906 |SGI511|/(|SGI511| + TP5) 0.4951 HIF521 2.0161 HIF521/HOI 0.6110 SGI521 0.7070 |SGI521|/(|SGI521| + TP5) 0.5400 HIF611 0.8192 HIF611/HOI 0.2482 SGI611 0.0146 |SGI611|/(|SGI611| + TP6) 0.0197 HIF621 2.4022 HIF621/HOI 0.7280 SGI621 −0.3221 |SGI621|/(|SGI621| + TP6) 0.3071 HIF711 0.1649 HIF711/HOI 0.0500 SGI711 0.0004 |SGI711|/(|SGI711| + TP7) 0.0011 HIF712 1.8319 HIF712/HOI 0.5551 SGI712 −0.3594 |SGI712|/(|SGI712| + TP7) 0.5004 HIF721 0.5635 HIF721/HOI 0.1708 SGI721 0.0381 |SGI721|/(|SGI721| + TP7) 0.0960 HIF722 2.6593 HIF722/HOI 0.8058 SGI722 −0.1949 |SGI722|/(|SGI722| + TP7) 0.3520

Fifth Embodiment

As shown in FIG. 5A and FIG. 5B, an optical image capturing system 50 of the fifth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 510, an aperture 500, a second lens 520, a third lens 530, a fourth lens 540, a fifth lens 550, a sixth lens 560, a seventh lens 570, an infrared rays filter 580, an image plane specifically for the infrared light 590, and an image sensor 592. FIG. 5C shows a modulation transformation of the optical image capturing system 50 of the fifth embodiment of the present application in infrared spectrum, and FIG. 5D shows a modulation transformation of the optical image capturing system 50 of the fifth embodiment of the present application in infrared spectrum.

The first lens 510 has positive refractive power and is made of plastic. An object-side surface 512, which faces the object side, is a convex aspheric surface, and an image-side surface 514, which faces the image side, is a concave aspheric surface. The object-side surface 512 has two inflection points, and the image-side surface 514 has three inflection points.

The second lens 520 has negative refractive power and is made of plastic. An object-side surface 522 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 524 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 522 has an inflection point, and the image-side surface 524 has three inflection points.

The third lens 530 has negative refractive power and is made of plastic. An object-side surface 532, which faces the object side, is a concave aspheric surface, and an image-side surface 534, which faces the image side, is a convex aspheric surface. The object-side surface 532 has an inflection point, and the image-side surface 534 has two inflection points.

The fourth lens 540 has negative refractive power and is made of plastic. An object-side surface 542, which faces the object side, is a convex aspheric surface, and an image-side surface 544, which faces the image side, is a concave aspheric surface. The object-side surface 542 has an inflection point, and the image-side surface 544 has three inflection points.

The fifth lens 550 has positive refractive power and is made of plastic. An object-side surface 552, which faces the object side, is a convex aspheric surface, and an image-side surface 554, which faces the image side, is a concave aspheric surface. The object-side surface 552 and the image-side surface 554 both have an inflection point.

The sixth lens 560 has positive refractive power and is made of plastic. An object-side surface 562, which faces the object side, is a convex aspheric surface, and an image-side surface 564, which faces the image side, is a convex aspheric surface. The object-side surface 562 has an inflection point, and the image-side surface 564 has two inflection points. Whereby, the incident angle of each view field entering the sixth lens 560 can be effectively adjusted to improve aberration.

The seventh lens 570 has negative refractive power and is made of plastic. An object-side surface 572, which faces the object side, is a concave aspheric surface, and an image-side surface 574, which faces the image side, is a concave aspheric surface. The object-side surface 572 has an inflection point, and the image-side surface 574 has two inflection points. It may help to shorten the back focal length to keep small in size. In addition, it could effectively suppress the incidence angle of light in the off-axis view field, and correct the off-axis view field aberration.

The infrared rays filter 580 is made of glass and between the seventh lens 570 and the image plane specifically for the infrared light 590. The infrared rays filter 580 gives no contribution to the focal length of the system.

The parameters of the lenses of the fifth embodiment are listed in Table 9 and Table 10.

TABLE 9 f = 6.7546 mm; f/HEP = 1.0; HAF = 25.7508 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 5.298245424 0.803 plastic 1.584 29.89 11.921 2 21.57523391 1.000 3 Aperture 1E+18 −0.697  4 2^(nd) lens 23.40585276 1.040 plastic 1.515 56.55 −95.106 5 15.57045994 0.881 6 3^(rd) lens −2.992855613 0.664 plastic 1.661 20.39 −104.018 7 −3.405383503 0.050 8 4^(th) lens 2.574574018 0.628 plastic 1.544 56.09 −29.561 9 2.027728857 0.064 10 5^(th) lens 2.123128122 0.769 plastic 1.661 20.39 8.130 11 3.033309022 1.437 12 6^(th) lens 22.79085785 0.793 plastic 1.661 20.39 9.104 13 −7.9244487 0.687 14 7^(th) lens −30.54121414 0.350 plastic 1.636 23.89 −7.193 15 5.32930708 0.215 16 Infrared rays 1E+18 0.215 BK_7 1.517 64.2 filter 17 1E+18 0.999 18 Image plane 1E+18 0.000 specifically for infrared light Reference wavelength: 940 nm; the position of blocking light: the effective half diameter of the clear aperture of the first surface is 3.850 mm; the effective half diameter of the clear aperture of the sixth surface is 3.468 mm; the effective half diameter of the clear aperture of the seventh surface is 3.468 mm; the effective half diameter of the clear aperture of the fifteenth surface is 3.220 mm; the exit pupil diameter of the image-side surface of the seventh lens is used as HXP

TABLE 10 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −5.245636E+00 −8.053831E+01 3.783436E+01 −8.999849E+01 −1.073550E+01 −1.270020E+01 −1.088205E+00 A4  1.928599E−03  4.942448E−03 8.338823E−03  3.456488E−03 −3.712552E−03 −9.643133E−03 −1.835446E−02 A6 −7.897549E−04 −2.857701E−03 −3.761874E−03  −3.046736E−03  1.016865E−03  3.333087E−03  4.894732E−03 A8  2.638472E−05  7.173579E−04 1.181456E−03  9.194580E−04 −7.610935E−05 −6.447460E−04 −1.365563E−03 A10 −3.719980E−06 −1.008558E−04 −1.824933E−04  −1.645991E−04 −1.441722E−06  9.187533E−05  2.596052E−04 A12  7.864408E−07  7.947799E−06 1.524817E−05  1.721252E−05  1.140757E−06 −8.327670E−06 −2.908487E−05 A14 −5.082501E−08 −3.254641E−07 −6.731053E−07  −9.315642E−07 −8.523554E−08  4.114781E−07  1.900000E−06 A16  1.061118E−09  5.381534E−09 1.206802E−08  1.987826E−08  1.763176E−09 −8.500219E−09 −5.878333E−08 Surface 9 10 11 12 13 14 15 k −4.861370E+00 −3.151498E+00 −1.380852E−01 −8.999002E+01 −3.395831E+01  8.997881E+01 −1.540630E+01 A4  1.847371E−02  1.578337E−02 −2.802058E−03  1.765631E−03 −6.166059E−03 −5.367681E−02 −4.350907E−02 A6 −2.085130E−02 −1.170561E−02  2.986950E−03  4.956375E−04  4.293549E−03  2.087925E−02  1.701734E−02 A8  7.418098E−03  4.139603E−03 −1.100715E−03 −7.708985E−05 −1.164607E−03 −5.302619E−03 −4.505894E−03 A10 −1.415525E−03 −7.914835E−04  1.035897E−04 −1.081823E−05  2.277156E−04  8.425794E−04  7.588408E−04 A12  1.595465E−04  8.848275E−05  1.196524E−05  7.453158E−06 −2.269772E−05 −7.110360E−05 −7.720766E−05 A14 −9.837656E−06 −5.393224E−06 −2.975898E−06 −1.663596E−06  6.409401E−07  2.703230E−06  4.339745E−06 A16  2.496134E−07  1.295827E−07  1.462739E−07  9.358254E−08  1.544011E−08 −2.783714E−08 −1.029223E−07

An equation of the aspheric surfaces of the fifth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the fifth embodiment based on Table 9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 940 nm) MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.88  0.87  0.81  0.74  0.71  0.63  ETP1 ETP2 ETP3 ETP4 ETP5 ETP6 0.496 0.729 0.662 0.418 0.832 0.653 ETP7 ETL EBL EIN EIR PIR 0.780 9.472 1.483 7.990 0.268 0.215 EIN/ETL SETP/EIN EIR/PIR SETP STP SETP/STP 0.843 0.572 1.245 4.569 5.048 0.905 ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.618 0.701 0.996 0.665 1.081 0.824 ETP7/TP7 BL EBL/BL SED SIN SED/SIN 2.228 1.265  1.1723 3.420 3.422 0.999 ED12 ED23 ED34 ED45 ED56 ED67 0.587 0.218 1.671 0.450 0.153 0.342 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56 ED67/IN67 1.942 0.247 33.413  7.032 0.106 0.497 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6|  0.5666  0.0710  0.0649  0.2285  0.8308  0.7420 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f  0.9391  1.6020  1.8409  0.8702  0.0448  0.1017 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6  0.1253  0.9143 1.0637 1.3078 HOS InTL HOS/HOI InS/HOS ODT % TDT %  9.7349  8.4701  2.9500  0.8148  1.2770  0.5062 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32  2.8242 0    0     3.4212  2.8786 0    HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS  2.3264  2.0658  2.6379  1.4103  0.4274  0.1449 IN12 IN23 IN34 IN45 IN56 IN67 0.3024 mm 0.8814 mm 0.0500 mm 0.0639 mm 1.4372 mm 0.6872 mm

The results of the equations of the fifth embodiment based on Table 9 and Table 10 are listed in the following table:

Values related to the inflection points of the fifth embodiment (Reference wavelength: 940 nm) HIF111 1.7198 HIF111/HOI 0.5212 SGI111 0.2515 |SGI111|/(|SGI111| + TP1) 0.2384 HIF112 3.8276 HIF112/HOI 1.1599 SGI112 0.2909 |SGI112|/(|SGI112| + TP1) 0.2658 HIF121 1.6129 HIF121/HOI 0.4887 SGI121 0.0609 |SGI121|/(|SGI121| + TP1) 0.0705 HIF122 3.0770 HIF122/HOI 0.9324 SGI122 0.1294 |SGI122|/(|SGI122| + TP1) 0.1387 HIF123 3.5286 HIF123/HOI 1.0693 SGI123 0.1413 |SGI123|/(|SGI123| + TP1) 0.1496 HIF211 3.0150 HIF211/HOI 0.9136 SGI211 0.5603 |SGI211|/(|SGI211| + TP2) 0.3502 HIF221 1.2598 HIF221/HOI 0.3818 SGI221 0.0461 |SGI221|/(|SGI221l + TP2) 0.0425 HIF222 2.4869 HIF222/HOI 0.7536 SGI222 0.0921 |SGI222|/(|SGI222| + TP2) 0.0814 HIF223 3.1621 HIF223/HOI 0.9582 SGI223 0.1214 |SGI223|/(|SGI223| + TP2) 0.1046 HIF311 1.7161 HIF311/HOI 0.5200 SGI311 −0.3344 |SGI311|/(|SGI311| + TP3) 0.3348 HIF321 1.7553 HIF321/HOI 0.5319 SGI321 −0.3317 |SGI321|/(|SGI321| + TP3) 0.3329 HIF322 3.1435 HIF322/HOI 0.9526 SGI322 −0.6300 |SGI322|/(|SGI322| + TP3) 0.4867 HIF411 2.7914 HIF411/HOI 0.8459 SGI411 1.1052 |SGI411|/(|SGI411| + TP4) 0.6376 HIF421 1.1380 HIF421/HOI 0.3449 SGI421 0.2587 |SGI421|/(|SGI421| + TP4) 0.2917 HIF422 1.8434 HIF422/HOI 0.5586 SGI422 0.4914 |SGI422|/(|SGI422| + TP4) 0.4389 HIF423 2.6897 HIF423/HOI 0.8151 SGI423 0.8243 |SGI423|/(|SGI423| + TP4) 0.5675 HIF511 2.4656 HIF511/HOI 0.7471 SGI511 1.0510 |SGI511|/(|SGI511| + TP5) 0.5774 HIF521 2.3776 HIF521/HOI 0.7205 SGI521 1.0234 |SGI521|/(|SGI521| + TP5) 0.5709 HIF611 1.9504 HIF611/HOI 0.5910 SGI611 0.1086 |SGI611|/(|SGI611| + TP6) 0.1205 HIF621 1.2702 HIF621/HOI 0.3849 SGI621 −0.0901 |SGI621|/(|SGI621| + TP6) 0.1020 HIF622 2.3880 HIF622/HOI 0.7236 SGI622 −0.1403 |SGI622|/(|SGI622| + TP6) 0.1503 HIF711 1.9336 HIF711/HOI 0.5859 SGI711 −0.3155 |SGI711|/(|SGI711| + TP7) 0.4741 HIF721 0.6339 HIF721/HOI 0.1921 SGI721 0.0299 |SGI721|/(|SGI721| + TP7) 0.0788 HIF722 2.5154 HIF722/HOI 0.7623 SGI722 −0.0251 |SGI722|/(|SGI722| + TP7) 0.0669

Sixth Embodiment

As shown in FIG. 6A and FIG. 6B, an optical image capturing system 60 of the sixth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 610, an aperture 600, a second lens 620, a third lens 630, a fourth lens 640, a fifth lens 650, a sixth lens 660, a seventh lens 670, an infrared rays filter 680, an image plane specifically for the infrared light 690, and an image sensor 692. FIG. 6C shows a modulation transformation of the optical image capturing system 60 of the sixth embodiment of the present application in infrared spectrum.

The first lens 610 has positive refractive power and is made of plastic. An object-side surface 612, which faces the object side, is a convex aspheric surface, and an image-side surface 614, which faces the image side, is a concave aspheric surface. The object-side surface 612 and the image-side surface 614 both have two inflection points.

The second lens 620 has negative refractive power and is made of plastic. An object-side surface 622 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 624 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 622 and the image-side surface 624 both have an inflection point.

The third lens 630 has positive refractive power and is made of plastic. An object-side surface 632, which faces the object side, is a convex aspheric surface, and an image-side surface 634, which faces the image side, is a concave aspheric surface. The object-side surface 632 has two inflection points, and the image-side surface 634 has an inflection point.

The fourth lens 640 has positive refractive power and is made of plastic. An object-side surface 642, which faces the object side, is a convex aspheric surface, and an image-side surface 644, which faces the image side, is a concave aspheric surface. The object-side surface 642 and the image-side surface 644 both have two inflection points.

The fifth lens 650 has positive refractive power and is made of plastic. An object-side surface 652, which faces the object side, is a convex aspheric surface, and an image-side surface 654, which faces the image side, is a concave aspheric surface. The object-side surface 652 and the image-side surface 654 both have an inflection point.

The sixth lens 660 has positive refractive power and is made of plastic. An object-side surface 662, which faces the object side, is a concave aspheric surface, and an image-side surface 664, which faces the image side, is a convex aspheric surface. The object-side surface 662 has an inflection point, and the image-side surface 664 has two inflection points. Whereby, the incident angle of each view field entering the sixth lens 660 can be effectively adjusted to improve aberration.

The seventh lens 670 has negative refractive power and is made of plastic. An object-side surface 672, which faces the object side, is a convex aspheric surface, and an image-side surface 674, which faces the image side, is a concave aspheric surface. The object-side surface 672 has an inflection point, and the image-side surface 674 has two inflection points. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 680 is made of glass and between the seventh lens 670 and the image plane specifically for the infrared light 690. The infrared rays filter 680 gives no contribution to the focal length of the system.

The parameters of the lenses of the sixth embodiment are listed in Table 11 and Table 12.

TABLE 11 f = 5.4554 mm; f/HEP = 1.0; HAF = 30.7306 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 7.403214857 0.636 plastic 1.661 20.39 16.166 2 23.98518038 0.492 3 Aperture 1E+18 −0.192  4 2^(nd) lens 27.4566196 0.502 plastic 1.535 56.27 −9.745 5 4.332797437 0.141 6 3^(rd) lens 4.806045993 1.216 plastic 1.661 20.39 95.528 7 4.68719334 0.025 8 4^(th) lens 1.919925537 0.404 plastic 1.661 20.39 183.635 9 1.789112884 0.195 10 5 ^(th) lens 1.629179352 0.794 plastic 1.661 20.39 4.794 11 2.745525008 1.360 12 6^(th) lens −15.5607797 1.103 plastic 1.661 20.39 3.090 13 −1.835123842 0.058 14 7^(th) lens 4.668747528 0.496 plastic 1.636 23.89 −3.411 15 1.408817508 0.555 16 Infrared rays 1E+18 0.215 BK_7 1.517 64.2 filter 17 1E+18 1.000 18 Image plane 1E+18 0.000 specifically for infrared light Reference wavelength: 940 nm; the position of blocking light: the effective half diameter of the clear aperture of the sixth surface is 3.052 mm; the effective half diameter of the clear aperture of the seventh surface is 3.052 mm; the effective half diameter of the clear aperture of the fifteenth surface is 3.100 mm; the exit pupil diameter of the image-side surface of the seventh lens is used as HXP

TABLE 12 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −6.471522E+00 5.017512E+01 8.468561E+01 1.519050E−01 −5.849631E−01 −4.323861E+01 −1.757211E+00 A4 −1.909932E−03 2.464708E−03 6.877273E−03 2.028632E−02  3.324090E−02  3.829457E−02 −3.272666E−02 A6 −2.183382E−03 −1.658762E−03  3.504253E−03 −1.388918E−02  −1.792549E−02 −2.778540E−02  1.959961E−02 A8  3.649789E−04 9.385835E−05 −1.485691E−03  3.750999E−03  4.378395E−03  7.458736E−03 −7.161591E−03 A10 −3.103639E−05 −1.741197E−06  2.773940E−04 −6.050352E−04  −6.921896E−04 −1.152818E−03  1.291453E−03 A12  2.599034E−06 2.546850E−06 −3.323699E−05  5.085651E−05  6.335653E−05  1.062509E−04 −1.204098E−04 A14 −1.795986E−07 −3.539700E−07  2.441048E−06 −1.934188E−06  −2.833287E−06 −5.362706E−06  5.498825E−06 A16  5.397901E−09 1.307455E−08 −9.297826E−08  1.919408E−08  4.355499E−08  1.130535E−07 −9.041571E−08 Surface 9 10 11 12 13 14 15 k −4.449897E+00 −3.257344E+00 −6.344560E−02 −8.949906E+01 −5.814758E+00 −8.463555E+01 −7.439015E+00 A4 −3.315092E−02  8.706007E−03  1.968907E−02  3.833713E−03  1.024842E−02 −8.118480E−03 −2.173600E−02 A6  2.398266E−02 −9.662848E−05 −7.719420E−03  1.775964E−03 −1.218976E−02 −5.344868E−03  5.028822E−03 A8 −5.864643E−03 −1.825622E−03 −1.561896E−03 −2.571649E−03  6.468174E−03  2.793763E−03 −1.216120E−03 A10  5.288627E−04  1.007111E−03  1.266608E−03  1.287524E−03 −1.941318E−03 −6.347361E−04  2.135051E−04 A12  1.421727E−05 −2.261510E−04 −2.744341E−04 −2.919860E−04  3.690127E−04  7.790082E−05 −2.508976E−05 A14 −5.682184E−06  2.391817E−05  2.540394E−05  3.301279E−05 −3.734553E−05 −4.744222E−06  1.663485E−06 A16  2.790551E−07 −1.030034E−06 −9.176693E−07 −1.575743E−06  1.478237E−06  1.090987E−07 −4.480557E−08

An equation of the aspheric surfaces of the sixth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the sixth embodiment based on Table 11 and Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 940 nm) MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.75  0.67  0.51  0.52  0.44  0.19  ETP1 ETP2 ETP3 ETP4 ETP5 ETP6 0.536 0.622 0.664 0.518 0.596 0.728 ETP7 ETL EBL EIN EIR PIR 0.901 8.887 1.431 7.456 0.216 0.555 EIN/ETL SETP/EIN EIR/PIR SETP STP SETP/STP 0.839 0.612 0.388 4.566 5.151 0.886 ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ETP5/TP5 ETP6/TP6 0.843 1.239 0.546 1.284 0.751 0.659 ETP7/TP7 BL EBL/BL SED SIN SED/SIN 1.817 1.590 0.9  2.890 2.078 1.390 ED12 ED23 ED34 ED45 ED56 ED67 0.661 0.132 0.981 0.469 0.172 0.475 ED12/IN12 ED23/IN23 ED34/IN34 ED45/IN45 ED56/IN56 ED67/IN67 2.201 0.938 39.225  2.409 0.127 8.254 |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6|  0.3375  0.5598  0.0571  0.0297  1.1379  1.7654 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f  1.5996  3.3276  2.1594  1.5410  0.0550  0.0106 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6  1.6589  0.1020 1.8638 0.5016 HOS InTL HOS/HOI InS/HOS ODT % TDT %  8.8201  7.2297  2.6727  0.8721  1.7527  0.7735 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32  2.0395  1.8794  2.6201  2.4199  2.4397  1.6489 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS  1.6216  2.1706  1.2956  2.1187  0.6420  0.2402 IN12 IN23 IN34 IN45 IN56 IN67 0.3001 mm 0.1412 mm 0.0250 mm 0.1946 mm 1.3599 mm 0.0576 mm

The results of the equations of the sixth embodiment based on Table 11 and Table 12 are listed in the following table:

Values related to the inflection points of the sixth embodiment (Reference wavelength: 940 nm) HIF111 1.1749 HIF111/HOI 0.3560 SGI111 0.0820 |SGI111|/(|SGI111| + TP1) 0.1142 HIF112 2.6747 HIF112/HOI 0.8105 SGI112 0.1089 |SGI112|/(|SGI112| + TP1) 0.1462 HIF121 1.2408 HIF121/HOI 0.3760 SGI121 0.0336 |SGI121|/(|SGI121| + TP1) 0.0502 HIF122 2.5783 HIF122/HOI 0.7813 SGI122 0.0180 |SGI122|/(|SGI122| + TP1) 0.0275 HIF211 2.1407 HIF211/HOI 0.6487 SGI211 0.2634 |SGI211|/(|SGI211| + TP2) 0.3440 HIF221 1.6341 HIF221/HOI 0.4952 SGI221 0.3273 |SGI221|/(|SGI221| + TP2) 0.3946 HIF311 1.5162 HIF311/HOI 0.4595 SGI311 0.2859 |SGI311|/(|SGI311| + TP3) 0.1903 HIF312 2.7512 HIF312/HOI 0.8337 SGI312 0.4723 |SGI312|/(|SGI312| + TP3) 0.2797 HIF321 0.9937 HIF321/HOI 0.3011 SGI321 0.0946 |SGI321|/(|SGI321| + TP3) 0.0722 HIF411 1.5056 HIF411/HOI 0.4562 SGI411 0.4677 |SGI411|/(|SGI411| + TP4) 0.5366 HIF412 2.4486 HIF412/HOI 0.7420 SGI412 0.8386 |SGI412|/(|SGI412| + TP4) 0.6749 HIF421 1.9207 HIF421/HOI 0.5820 SGI421 0.6588 |SGI421|/(|SGI421| + TP4) 0.6200 HIF422 2.7963 HIF422/HOI 0.8474 SGI422 1.0419 |SGI422|/(|SGI422| + TP4) 0.7207 HIF511 2.1788 HIF511/HOI 0.6603 SGI511 1.0304 |SGI511|/(|SGI511| + TP5) 0.5648 HIF521 2.0340 HIF521/HOI 0.6164 SGI521 0.8280 |SGI521|/(|SGI521| + TP5) 0.5105 HIF611 1.0243 HIF611/HOI 0.3104 SGI611 −0.0265 |SGI611|/(|SGI611| + TP6) 0.0235 HIF612 2.2118 HIF612/HOI 0.6702 SGI612 0.0111 |SGI612|/(|SGI612| + TP6) 0.0099 HIF621 1.4424 HIF621/HOI 0.4371 SGI621 −0.3745 |SGI621|/(|SGI621| + TP6) 0.2534 HIF622 2.4861 HIF622/HOI 0.7534 SGI622 −0.5198 |SGI622|/(|SGI622| + TP6) 0.3202 HIF711 0.6244 HIF711/HOI 0.1892 SGI711 0.0309 |SGI711|/(|SGI711| + TP7) 0.0586 HIF712 2.1949 HIF712/HOI 0.6651 SGI712 −0.0179 |SGI712|/(|SGI712| + TP7) 0.0349 HIF713 2.9170 HIF713/HOI 0.8839 SGI713 −0.0366 |SGI713|/(|SGI713| + TP7) 0.0688 HIF721 0.8213 HIF721/HOI 0.2489 SGI721 0.1633 |SGI721|/(|SGI721| + TP7) 0.2477 HIF722 2.9374 HIF722/HOI 0.8901 SGI722 0.2348 |SGI722|/(|SGI722| + TP7) 0.3213

It must be pointed out that the embodiments described above are only some embodiments of the present invention. All equivalent structures which employ the concepts disclosed in this specification and the appended claims should fall within the scope of the present invention. 

What is claimed is:
 1. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane specifically for infrared light; wherein the optical image capturing system has a total of the seven lenses with refractive power; at least one lens among the first to the seventh lenses has positive refractive power; each lens of the first to the seventh lenses has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 0.5≤f/HEP≤1.8; 0 deg<HAF≤60 deg; and 0.5≤SETP/STP<1; wherein f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HAF is a half of a maximum field angle of the optical image capturing system; ETP1, ETP2, ETP3, ETP4, ETP5, ETP6, and ETP7 are respectively a thickness of the first lens, the second lens, the third lens, the fourth lens, the fifth lens, the sixth lens, and the seventh lens at a height of half of the exit pupil diameter away from the optical axis; SETP is a sum of the aforementioned ETP1 to ETP7; TP1, TP2, TP3, TP4, TP5, TP6, and TP7 are respectively a thickness of the first lens, the second lens, the third lens, the fourth lens, the fifth lens, the sixth lens, and the seventh lens on the optical axis; STP is a sum of the aforementioned TP1 to TP7.
 2. The optical image capturing system of claim 1, wherein a wavelength of the infrared light ranges from 700 nm to 1300 nm, and a first spatial frequency is denoted by SP1, which satisfies the following condition: SP1≤440 cycles/mm.
 3. The optical image capturing system of claim 1, wherein a wavelength of the infrared light ranges from 850 nm to 960 nm, and a first spatial frequency is denoted by SP1, which satisfies the following condition: SP1≤220 cycles/mm.
 4. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.2≤EIN/ETL<1; wherein ETL is a distance in parallel with the optical axis between a coordinate point at a height of half of the entrance pupil diameter away from the optical axis on the object-side surface of the first lens and the image plane specifically for infrared light; EIN is a distance in parallel with the optical axis between the coordinate point at the height of half of the entrance pupil diameter away from the optical axis on the object-side surface of the first lens and a coordinate point at a height of half of the entrance pupil diameter away from the optical axis on the image-side surface of the seventh lens.
 5. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.1≤EBL/BL≤1.5; wherein EBL is a horizontal distance in parallel with the optical axis between a coordinate point at a height of half of the entrance pupil diameter away from the optical axis on the image-side surface of the seventh lens and the image plane specifically for infrared light; BL is a horizontal distance in parallel with the optical axis between the point on the image-side surface of the seventh lens where the optical axis passes through and the image plane specifically for infrared light.
 6. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: IN56>IN23; wherein IN23 is a distance on the optical axis between the second lens and the third lens, and IN56 is a distance on the optical axis between the fifth lens and the sixth lens.
 7. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: IN56>IN34; wherein IN34 is a distance on the optical axis between the third lens and the fourth lens, and IN56 is a distance on the optical axis between the fifth lens and the sixth lens.
 8. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: IN56>IN45; wherein IN45 is a distance on the optical axis between the fourth lens and the fifth lens, and IN56 is a distance on the optical axis between the fifth lens and the sixth lens.
 9. The optical image capturing system of claim 1, further comprising an aperture, wherein the optical image capturing system further satisfies: 0.2≤InS/HOS≤1.1; wherein InS is a distance between the aperture and the image plane specifically for infrared light on the optical axis, and HOS is a distance between the object-side surface of the first lens and the image plane specifically for infrared light on the optical axis.
 10. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane specifically for infrared light; wherein the optical image capturing system has a total of seven lens with refractive power; at least one surface of at least one lens among the first lens to the seventh lens has at least an inflection point; at least one lens among the first lens to the seventh lens has positive refractive power; each lens among the first to the seventh lenses has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 0.5≤f/HEP≤1.5; 0 deg<HAF≤45 deg; and 0.2≤EIN/ETL<1; wherein f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HAF is a half of the maximum field angle of the optical image capturing system; ETL is a distance in parallel with the optical axis between a coordinate point at a height of half of the entrance pupil diameter away from the optical axis on the object-side surface of the first lens and the image plane specifically for infrared light; EIN is a distance in parallel with the optical axis between the coordinate point at the height of half of the entrance pupil diameter away from the optical axis on the object-side surface of the first lens and a coordinate point at height of half of the entrance pupil diameter away from the optical axis on the image-side surface of the seventh lens.
 11. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: MTFQ0≥0.01; MTFQ3≥0.01; and MTFQ7≥0.01 wherein MTFQ0, MTFQ3, and MTFQ7 are respectively values of modulation transfer function of infrared light in a spatial frequency of 110 cycles/mm at the optical axis, 0.3 HOI, and 0.7 HOI on the image plane specifically for infrared light.
 12. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: MTFE0≥0.01; MTFE3≥0.01; and MTFE7≥0.01 wherein MTFE0, MTFE3, and MTFE7 are respectively values of modulation transfer function of infrared light in a spatial frequency of 55 cycles/mm at the optical axis, 0.3 HOI, and 0.7 HOI on the image plane specifically for infrared light.
 13. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0.5≤HOS/HOI≤6; wherein HOS is a distance between the object-side surface of the first lens and the image plane specifically for infrared light on the optical axis; HOI is a maximum height for image formation perpendicular to the optical axis on the image plane specifically for infrared light.
 14. The optical image capturing system of claim 10, further comprising an aperture disposed before the image-side surface of the third lens.
 15. The optical image capturing system of claim 10, wherein the image-side surface of the first lens is concave on the optical axis.
 16. The optical image capturing system of claim 10, wherein the object-side surface of the second lens is convex on the optical axis.
 17. The optical image capturing system of claim 10, wherein the object-side surface of the fourth lens is convex on the optical axis, and the image-side surface of the fourth lens is concave on the optical axis.
 18. The optical image capturing system of claim 10, the object-side surface of the fifth lens is convex on the optical axis, and the image-side surface of the fifth lens is concave on the optical axis.
 19. The optical image capturing system of claim 10, wherein the first lens to the seventh lens are all made of plastic.
 20. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: an aperture; a first lens having refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane specifically for infrared light; wherein the optical image capturing system has a total of the seven lenses having refractive power; at least one surface of each of at least two lenses among the first lens to the seventh lens has at least an inflection point; each lens of the first to the seventh lenses has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 0.5≤f/HEP≤1.4; 0 deg<HAF≤30 deg; and 0.5≤SETP/STP<1; wherein f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HAF is a half of a maximum view angle of the optical image capturing system; ETP1, ETP2, ETP3, ETP4, ETP5, ETP6, and ETP7 are respectively a thickness of the first lens, the second lens, the third lens, the fourth lens, the fifth lens, the sixth lens, and the seventh lens at a height of half of the exit pupil diameter away from the optical axis; SETP is a sum of the aforementioned ETP1 to ETP7; TP1, TP2, TP3, TP4, TP5, TP6, and TP7 are respectively a thickness of the first lens, the second lens, the third lens, the fourth lens, the fifth lens, the sixth lens, and the seventh lens on the optical axis; STP is a sum of the aforementioned TP1 to TP7.
 21. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: 0 mm<HOS≤20 mm; wherein HOS is a distance between the object-side surface of the first lens and the image plane specifically for infrared light on the optical axis.
 22. The optical image capturing system of claim 20, wherein a wavelength of the infrared light ranges from 850 nm to 960 nm, and a first spatial frequency is denoted by SP1, which satisfies the following condition: SP1≤220 cycles/mm.
 23. The optical image capturing system of claim 20, wherein the first lens to the seventh lens are all made of plastic.
 24. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: IN56>IN23; IN56>IN34; and IN56>IN45; wherein IN23 is a distance on the optical axis between the second lens and the third lens, IN34 is a distance on the optical axis between the third lens and the fourth lens, IN45 is a distance on the optical axis between the fourth lens and the fifth lens, and IN56 is a distance on the optical axis between the fifth lens and the sixth lens.
 25. The optical image capturing system of claim 20, further comprising an aperture and an image sensor, wherein the optical image capturing system further satisfies: 0.2≤InS/HOS≤1.1; wherein the image sensor is disposed on the image plane specifically for infrared light and is provided with at least one hundred thousand pixels, and InS is a distance between the aperture and the image plane specifically for infrared light on the optical axis; HOS is a distance between the object-side surface of the first lens and the image plane specifically for infrared light on the optical axis. 